Electron-Phonon Interactions in Novel Nanoelectronics

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ELECTRON-PHONON INTERACTIONS IN NOVEL NANOELECTRONICS

No part of this digital document may be reproduced, stored in a retrieval system or transmitted in any form or by any means. The publisher has taken reasonable care in the preparation of this digital document, but makes no expressed or implied warranty of any kind and assumes no responsibility for any errors or omissions. No liability is assumed for incidental or consequential damages in connection with or arising out of information contained herein. This digital document is sold with the clear understanding that the publisher is not engaged in rendering legal, medical or any other professional services.

ELECTRON-PHONON INTERACTIONS IN NOVEL NANOELECTRONICS

TAKASHI KATO

Nova Science Publishers, Inc. New York

Copyright © 2009 by Nova Science Publishers, Inc.

All rights reserved. No part of this book may be reproduced, stored in a retrieval system or transmitted in any form or by any means: electronic, electrostatic, magnetic, tape, mechanical photocopying, recording or otherwise without the written permission of the Publisher. For permission to use material from this book please contact us: Telephone 631-231-7269; Fax 631-231-8175 Web Site: http://www.novapublishers.com NOTICE TO THE READER The Publisher has taken reasonable care in the preparation of this book, but makes no expressed or implied warranty of any kind and assumes no responsibility for any errors or omissions. No liability is assumed for incidental or consequential damages in connection with or arising out of information contained in this book. The Publisher shall not be liable for any special, consequential, or exemplary damages resulting, in whole or in part, from the readers’ use of, or reliance upon, this material. Independent verification should be sought for any data, advice or recommendations contained in this book. In addition, no responsibility is assumed by the publisher for any injury and/or damage to persons or property arising from any methods, products, instructions, ideas or otherwise contained in this publication. This publication is designed to provide accurate and authoritative information with regard to the subject matter covered herein. It is sold with the clear understanding that the Publisher is not engaged in rendering legal or any other professional services. If legal or any other expert assistance is required, the services of a competent person should be sought. FROM A DECLARATION OF PARTICIPANTS JOINTLY ADOPTED BY A COMMITTEE OF THE AMERICAN BAR ASSOCIATION AND A COMMITTEE OF PUBLISHERS. Library of Congress Cataloging-in-Publication Data ISBN: 978-1-61728-391-8 (E-Book) Available upon request

Published by Nova Science Publishers, Inc.   New York

CONTENTS Preface

vii

Chapter I

Introduction

1

Chapter II

Theoretical Background

5

Chapter III

Electron–Phonon Coupling Constants for the Charged Electronic States of Polyacenes, Polyfluoroacenes, B, N-Substituted Polyacenes, and Polycyanodienes

15

Chapter IV

Optimized Structures

21

Chapter V

Electron–Phonon Coupling Constants

27

Chapter VI

Total Electron–Phonon Coupling Constants

49

Chapter VII

The Logarithmically Averaged Phonon Frequencies

63

Chapter VIII

Concluding Remarks

73

Acknowledgment

77

References

79

Index

85

PREFACE In this book, the electron–phonon interactions in the charged molecular systems such as polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes are discussed. We estimated the electron–phonon coupling constants and the frequencies of the vibronic active modes playing an essential role in the electron–phonon interactions in order to discuss how CH–CF, CC–BN, and CC–CN substitutions are closely related to the essential characteristics of the electron–phonon interactions in these molecules by comparing the calculated results for charged polyacenes with those for charged B, N-substituted polyacenes and polycyanodienes, respectively. The C–C stretching modes around 1500 cm1 strongly couple to the highest occupied molecular orbitals (HOMO), and the lowest frequency modes and the C–C stretching modes around 1500 cm–1 strongly couple to the lowest unoccupied molecular orbitals (LUMO) in polyacenes. The C–C stretching modes around 1500 cm -1strongly couple to the HOMO and LUMO in polyfluoroacenes. The B–N stretching modes around 1500 cm -1 strongly couple to the HOMO and LUMO in B, N-substituted polyacenes. The C– C and C–N stretching modes around 1500 cm-1 strongly couple to the HOMO and LUMO in polycyanodienes. The total electron–phonon coupling constants for the monocations ( lHOMO ) and monoanions ( lLUMO ) decrease with an increase in molecular size in polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes. In general, we can expect that monocations and monoanions, in which number of carriers per atom is larger, affords larger value. The CH–CF, CC–BN, and CC–CN atomic substitutions are effective way to seek for larger lHOMO values, and the CH–CF and CC–CN atomic substitutions are effective way to seek for larger lLUMO values in polyacenes. The logarithmically averaged phonon frequencies ( ω ln ) which measure the frequencies of the vibronic active

viii

Takashi Kato

modes playing an essential role in the electron–phonon interactions for the monocations ( ω ln,HOMO ) and monoanions ( ω ln,LUMO ) in polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes are investigated. The ω ln,HOMO values decrease with an increase in molecular size in polyacenes, polyfluoroacenes, and polycyanodienes, and the ω ln,LUMO values decrease with an increase in molecular size in polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes. We can expect that in the hydrocarbon molecular systems, the ω ln values would basically decrease by substituting hydrogen atoms by heavier atoms. This can be understood from the fact that the frequencies of all vibronic active modes in polyacenes downshift by H–F substitution. However, considering that the ω ln value for the LUMO rather localized on carbon atoms in large sized polyfluoroacenes becomes larger by H–F substitution, we can expect that the ω ln value for a molecular orbital localized on carbon atoms has a possibility to increase by substituting hydrogen atoms by heavier atoms if the phase patterns of the molecular orbital do not significantly change by such atomic substitution. Therefore, the detailed properties of the vibrational modes and the electronic structures as well as the molecular weights are closely related to the frequencies of the vibronic active modes playing an important role in the electron–phonon interactions in the monoanions of polyfluoroacenes.

Chapter I

INTRODUCTION In modern physics and chemistry, the effects of vibronic interactions [1] and electron–phonon interactions [1–3] in molecules and crystals have been an important topic. Analysis of vibronic interaction [1–3] is important for the prediction of electronic control of nuclear motions in degenerate electronic systems. Application of vibronic interaction theory covers a large variety of research fields such as spectroscopy,[4] instability of molecular structure, electrical conductivity,[5] and superconductivity.[5, 6] Vibronic interactions in discrete molecules can be viewed as the coupling between frontier orbitals and molecular vibrations, while those in solids are the coupling between free electrons near the Fermi level and acoustic phonons. There is a close analogy between them. Electron–phonon coupling [1–3] is the consensus mechanism for attractive electron–electron interactions in the Bardeen–Cooper–Schrieffer (BCS) theory of superconductivity.[5,6] Since Little’s proposal for a possible molecular superconductor based on exciton mechanism,7 the superconductivity of molecular systems has been extensively investigated. Although such a unique mechanism has not yet been established, advances in design and synthesis of molecular systems have yielded a lot of BEDT-TTF-type organic superconductors, [8, 9] where BEDT-TTF is bis(ethylenedithio)tetrathiafulvalene. An inverse isotope effect due to substituting hydrogen by deuterium in organic superconductivity was observed by Saito et al.[10] Goddard et al. proposed that the mechanism for superconductivity of BEDT–TTF type organic molecules involves the coupling of charge transfer to the boat deformation mode.[11] It was found that the alkalidoped A3C60 complexes [12] exhibit superconducting transition temperatures (Tcs)

2

Takashi Kato

of more than 30 K (Ref. [13]) and 40 K under pressure.[14] In superconductivity in alkali-doped fullerenes,15 pure intramolecular Raman-active modes have been suggested to be important in a BCS-type [6] strong coupling scenario. It was proposed that the electron–phonon interactions dominate the charge transport in the crystals of naphthalene (C10H8) (2a), anthracene (3a), tetracene (4a), and pentacene (5a).[16–18] Interestingly, from a theoretical viewpoint, possible superconductivity of polyacene has been proposed.[19,20] Saito et al.[10] observed an inverse isotope effect due to substituting hydrogen by deuterium in organic superconductivity. It is important to consider how intramolecular or intermolecular vibrations play a role in the occurrence of superconductivity. If the intermolecular vibrations are important, the phononfrequency dependence of the transition temperature appears in the prefactor through Debye frequency in the formula for the superconducting transition temperatures (Tcs) in the Bardeen–Cooper–Schrieffer (BCS) theory so that the normal isotope effects are expected. If the intramolecular vibrations are important, the phonon-frequency dependence appears in the denominator of the expression for the electron–phonon coupling constant so that the inverse isotope effect can be expected in some cases. From the inverse isotope effect on deuterium substitution observed by Saito et al.,[10] we expect that such inverse isotope effects can be widely observed in molecular organic superconductors. The origin of such inverse isotope effects in organic superconductors has not yet been fully elucidated. Shortly after the discovery of superconductivity in palladium hydrides,[21] an isotope effect in Tc was found by Stritzker and Buckel.[22] The Tc of Pd-D was higher than that of Pd-H,[23] contrary to the expectations from a simple BCS theory After that, an even larger inverse isotope effect for Pd-T was measured by Schirber et al.[24] In previous work, we have analyzed the vibronic interactions and estimated possible Tcs in the monocations of polyacenes based on the hypothesis that the vibronic interactions between the intramolecular vibrations and the highest occupied molecular orbitals (HOMO) play an essential role in the occurrence of superconductivity in positively charged nanosized molecular systems.[25] On the basis of an experimental study of ionization spectra using the highresolution gas-phase photoelectron spectroscopy, the electron–phonon interactions in the positively charged polyacenes were well studied recently.[26] Our predicted frequencies for the vibrational modes which play an essential role in the electron–phonon interactions [25] as well as the predicted total electron– phonon coupling constants [25] are in excellent agreement with those obtained from the experimental research.[26]

Introduction

1a

2a

3

4a

3a

5a

1fa

6a

3fa

2fa

4fa

1bn

1cn

5fa

3bn

2bn

3cn

2cn

4cn Scheme 1.

4

Takashi Kato

In this book, we discuss the electron–phonon interactions in the charged molecular systems such as polyacenes such as C6H6 (1a), C10H8 (2a), C14H10 (3a), C18H12 (4a), and C22H14 (5a),[25] polyfluoroacenes such as C6F6 (1fa), C10F8 (2fa), C14F10 (3fa), C18F12 (4fa), and C22F14 (5fa),[27] B, N-substituted polyacenes such as B3N3H6 (1bn), B5N5H8 (2bn), B7N7H10 (3bn),[28] and polycyanodienes such as C4N2H6 (1cn), C6N4H8 (2cn), C8N6H10 (3cn), and C10N8H12 (4cn)[29] (Scheme 1). We will estimate the electron–phonon coupling constants and the frequencies of the vibronic active modes playing an essential role in the electron–phonon interactions. These physical values are essential to discuss the several physical phenomena such as intramolecular electrical conductivity, intermolecular charge transfer, attractive electron–electron interactions and Bose–Einstein condensation, and superconductivity, which will be discussed in detail in the next review article. Motivated by the possible inverse isotope effects in Pd-H, Pd-D, and Pd-T superconductivity [21–24] and organic superconductivity observed by Saito et al.,[10] we discuss how the H–F substitution are closely related to the essential characteristics of the electron–phonon interactions in these molecules by comparing the calculated results for charged polyacenes with those for charged polyfluoroacenes, since fluorine atoms are much heavier than D and T atoms, and the phase patterns of the frontier orbitals such as the HOMO and LUMO are not expected to be significantly changed. Furthermore, we discuss how C–BN and C– N substitutions are closely related to the essential characteristics of the electron– phonon interactions in these molecules by comparing the calculated results for charged polyacenes with those for charged B, N-substituted polyacenes and polycyanodienes, respectively. We can expect that the characteristics of electron– phonon interactions are significantly changed by such atomic substitutions because of electronegativity perturbation30 in polyacenes. These physical values are essential to discuss the several physical phenomena such as intramolecular electrical conductivity, intermolecular charge transfer, attractive electron–electron interactions and Bose–Einstein condensation, and superconductivity, which will be discussed in detail in the next review article.

Chapter II

THEORETICAL BACKGROUND We describe the theoretical background for the vibronic coupling in polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes. We will use small letters for “one-electron orbital symmetries” and capital letters for symmetries of both “electronic” and “vibrational” states, as usual. The vibronic matrix element, Exy (r,Q) ,[1–3] is given by ⎛ ∂ 2 ε xy ⎞ ⎛ ∂ε xy ⎞ 1 ⎟ Qα + ∑ ⎜ = ∑⎜ ⎟ Q Q 2 α ,β ⎝ ∂Qα ∂Qβ ⎠ α β Exy (r,Q ) = ε xy (r,Q ) – ε xy (r,0 ) α ⎝ ∂ Qα ⎠ 0 0

(1)

where ε xy (r,Q) is defined as ε xy (r,Q) = φ x h(r,Q) φ y

(2)

Here, h(r,Q) is the Hamiltonian of one-electron orbital energy, and φ x and φ y are one-electron wave functions. r and Q signify the whole set of coordinates of the electrons and nuclei, respectively. What we see in the first term on the righthand side of Eq. (1) is the linear orbital vibronic coupling constant. We discuss a theoretical background for the orbital vibronic interactions in polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes. The potential energy for the neutral ground state, negatively and positively charged electronic states in polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes are shown in Figure 1. Here, we take a one-

Takashi Kato

6

electron approximation into account; the vibronic coupling constants of the vibrational modes to the electronic states in the monoanions and cations of polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes are defined as a sum of orbital vibronic coupling constants from all the occupied orbitals, [1(a)] gelectronic state =

occupied

∑ gi i

.

(3)

(a) Ground states in neutral polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes (A1 g ) (A1g ) ε ε m HOMO(1) εm HOMO(2 )

Q A1g m

(b) The monocations of1a, 1fa, and 1bn ε

(E2 g )

(A1 g )

(A1 g )

ε ε m HOMO(1) ε m HOMO(2 )

(E2g )

εm HOMO(1) ε m HOMO(2 )

QE 2 g ε m

Q A1g m

(c) The monocations of D 2h symmetric polyacenes, polyfluoroacenes, and polycyanodienes, an C2v symmetric B, N-substituted polyacenes ε

( g) εm HOMO A

Q Ag m

Figure 1. Potential energy for the neutral ground state and positively charged electronic states in polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes.


7

Considering the one-electron approximation and that the first derivatives of the total energy vanish in the ground state at the equilibrium structure in neutral polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes (i.e., gneutral =

HOMO

∑ gi = 0 ) (Figure 1 (a)), and one electron must be injected into i

(removed from) the LUMO (HOMO) to generate the monoanions (monocations), the vibronic coupling constants of the totally symmetric vibrational modes to the electronic states of the monoanions and cations of polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes can be defined by Eqs. (4) and (5), respectively, gmonoanion (ω m ) = gLUMO (ω m ),

(4)

gmonocation (ω m ) = gHOMO (ω m ) .

(5)

A. Vibronic Interactions between the Twofold Degenerate Frontier Orbitals and the E2g Vibrational Modes In Benzene Benzene (1a) has the twofold degenerate HOMO and LUMO due to its high D6h symmetry. The symmetry labels of the HOMO and LUMO are e1g and e2u, respectively. Now we take two approximations into account in Eq. (1). First, we ignore the nondiagonal matrix elements containing the quadratic vibronic constants; only the terms of type Qα2 are taken into account. Second, we focus upon the diagonal processes; we consider the direct product of the orbital symmetries, which can be reduced as e1g × e1g = e2u × e2u = A1g + A2g + E2g

.

(6)

Thus, the A1g and E2g modes can linearly couple to the e1g HOMO and e2u LUMO. The numbers of the A1g and E2g modes are 2 and 4, respectively. We must consider multimode problems, but in the limit of linear vibronic coupling we can treat each twofold degenerate set of modes (mode index m as shown below) independently.[1] Let us first consider the orbital vibronic coupling of the twofold degenerate e1g HOMO to the E2g vibrational mode. Taking two approximations mentioned

Takashi Kato

8

above and Eq. (1) into account, the two energy sheets of the e1g HOMO that can couple to the mth E2g vibrational mode are given in the form of Eq. (7), where QE γm is the vibrational normal coordinate belonging to row γ of the vibrational 2g

mode of the irreducible representation E2g:

(E2g ) Q

ε mxy

=

(

E2 gθ m , QE2 g εm

)

⎛ 1 ∂h ⎞ 2 K Q δ + e HOMO ⎜ ∑ ⎟ e1g y HOMO QE2g γ m E2g m E2g γ m xy ∑ 1g x 2 γ ⎝ ∂QE2 g γm ⎠ 0 γ

(m = 1,2,..., 4)

(7)

Here, γ takes two vibrational states θ and ε . The first term on the right-hand side of Eq. (7) is the elastic term, and

⎛ ∂h ⎞ e1g x HOMO ⎜ ⎟ e1g y HOMO ⎝ ∂QE2 g γm ⎠ 0

in the

second term corresponds to the linear orbital vibronic coupling constant, which is a good measure of the interaction between the vibration labeled by γ in the mth mode of the irreducible representation E2g and the molecular orbitals labeled by x and y in the irreducible representation e1g. According to the Wigner–Eckart theorem, [1] we can rewrite the second term on the right-hand side of Eq. (7) using the Clebsch–Gordan coefficients and we obtain the vibronic coupling matrix1 as ⎛ – QE2 gε m Q E2g θm ⎞ ⎟ QE2 gε m ⎠

ε E2g m = Am ⎜ Q ⎝ E2 gθ m

,

(8)

where Am corresponds to the reduced matrix element for the mth mode of vibration: ⎛ ∂h ⎞ Am = e1g HOMO ⎜ ⎟ e1g HOMO ⎝ ∂QE2 g m ⎠ 0

(9)

Am depends on the irreducible representation and not on rows. Using Eq. (8),

Eq. (7) can be transformed into Eq. (10):


(E2g ) Q

εm

(

E2 gθ m ,Q E2 g εm

)= 12 K (Q E2g m

2 E2g θm

9

⎛ –QE2g ε m ⎛⎜ 1 0⎞ 2 ⎜ + A + QE ε m m 2g ⎝ 0 1⎠ ⎝ QE2 gθm

)

QE2 gθ m ⎞ ⎟ QE2g ε m ⎠

(10) Now we consider one member of the twofold degenerate vibrational mode. For example, when we consider only the QE εm mode ( QE θ m = 0 ), the energy 2g

2g

sheets of the molecular orbital in row ε of the mth mode become

(E2g ) Q

εm

(

)

E2 g εm =

0 ⎞ ⎛ –QE2 gε m ⎛ 1 0⎞ 1 ⎟ + Am ⎜ K E2g mQ2E2g ε m ⎜ 0 QE2g ε m ⎠ ⎝ 0 1⎠ 2 ⎝

(11)

This has already been diagonalized, and the energy sheets of the molecular orbital (HOMO (1) and HOMO (2)) in row ε cut by the plane QE θ m = 0 become 2g

(E2g )

(

)

1 2

(12)

(

)

1 2

(13)

ε m HOMO (1) Q E2g ε m = K E2 gm QE22 gε m + Am QE2 gε m

and

(E2g )

ε m HOMO (2 ) QE2 g εm = K E2g mQ E2 2g ε m – AmQE2 g εm QE2 gθ m = 0

.

(14)

These are illustrated in Figure 1. Only the cases where the quadratic vibronic constants are positive are shown as examples here. We see from this illustration that the E2g modes lift the degeneracy of the twofold degenerate orbitals. The dimensionless diagonal linear orbital vibronic coupling constants of the e1g HOMO for its mth mode is defined by Eq. (15). ge1g HOMO (ω m ) =

⎛ ∂h ⎞ e1g HOMO ⎜ ⎟ e1g HOMO ωm ⎝ ∂q E2 g m ⎠ 0 1

(15)

In these equations, q E m is the dimensionless normal coordinate [31] defined 2g by

Takashi Kato

10 q E2g m = ω m / QE2 gm

(16)

Similar discussions can be made in the vibronic interactions between the E2g modes and the e2u LUMO, and the dimensionless diagonal linear orbital vibronic coupling constants of the e2u LUMO for the mth mode is defined by ge2 u LUMO (ω m ) =

⎛ ∂h ⎞ e2u LUMO ⎜ ⎟ e2u LUMO ωm ⎝ ∂qE2 g m ⎠ 0 1

(17)

B. Vibronic Interactions between the Twofold Degenerate Frontier Orbitals and the A1g Vibrational Modes in Benzene In this case, the two energy sheets of the molecular orbitals are given in the form:

(A1g ) Q

εm

( )= 12 K A1g m

0 ⎞ ⎛ Q A1g m ⎟ + Bm ⎜ 0 QA1 gm ⎠ ⎝ 0 1⎠ ⎝

⎛⎜ 1 2 A1g m QA1g m

0⎞

(18)

where Bm corresponds to the reduced matrix element written as ⎛ ∂h ⎞ Bm = e1g HOMO ⎜ ⎟ e1g HOMO ⎝ ∂ QA1g m ⎠ 0

(19)

This has already been diagonalized, and the energy sheets of the molecular orbital (HOMO (1) and HOMO (2)) become

(A1g )

(

)

(A1g )

(

)

1 2

ε m HOMO (1) QA1g m = ε m HOMO (2) QA1g m = K A1g mQA21gm + BmQA1 gm (20) These are illustrated in Figure 1. We can see from this illustration that the A1g modes do not lift the degeneracy of the twofold degenerate orbitals. The


11

dimensionless diagonal linear orbital vibronic coupling constants of the e1g HOMO for its mth mode is defined by Eq. (21),

ge1g HOMO (ω m ) =

⎛ ∂h ⎞ e1g HOMO ⎜ ⎟ e1g HOMO ωm ⎝ ∂q A1gm ⎠ 0 1

(21)

In this equation, q A m is the dimensionless normal coordinate [31] of the mth 1g mode defined by using the normal coordinate QA m as 1g q A1gm = ω m / QA1gm

(22)

In a similar way, the dimensionless diagonal linear orbital vibronic coupling constants of the e2u LUMO for the mth mode is defined by Eq. (23), ge2 u LUMO (ω m ) =

⎛ ∂h ⎞ e2u LUMO ⎜ ⎟ e2 u LUMO ωm ⎝ ∂q A1gm ⎠ 0 1

(23)

C. Vibronic Interactions between the Nondegenerate Frontier Orbitals and the Ag Vibrational Modes in Polyacenes Let us look into orbital vibronic coupling in polyacenes that have D2h geometries, and the nondegenerate HOMOs and LUMOs, the symmetry labels of the HOMOs (LUMOs) of 2a, 4a, and 6a being au (b1g) and those of 3a and 5a being b2g (b3u). Thus, the direct product of the HOMOs (LUMOs) symmetries can be reduced as au × au = b2 g × b2 g = b1g × b1g = b3u × b3u = Ag

(24)

Therefore, the totally symmetric Ag modes of vibration couple to the HOMOs (LUMOs). The numbers of the Ag vibrational modes are 9, 12, 15, 18, and 21 for 2a, 3a, 4a, 5a, and 6a, respectively. The symmetry labels of nondegenerate

Takashi Kato

12

frontier orbitals of these polyacenes are abbreviated as “a” in the following discussion. The energy sheet of the HOMO is given in the form:

(Ag )

( )

1 2

ε m HOMO QAg m = K Ag mQA2g m + CmQAg m

(25)

where Cm corresponds to the reduced matrix element written as ⎛ ∂h ⎞ Cm = a HOMO ⎜ ⎟ a HOMO ⎝ ∂ QAg m ⎠ 0

(26)

This is illustrated in Figure 1. The dimensionless diagonal linear orbital vibronic coupling constants of the HOMO for its mth mode is defined by Eq. (27),

ga HOMO (ω m ) =

⎛ ∂h ⎞ a HOMO ⎜ ⎟ a HOMO ωm ⎝ ∂q Agm ⎠ 0 1

(27)

In this equation, q A m is the dimensionless normal coordinate [31] of the mth g mode defined by using the normal coordinate QA m as g q Agm = ω m / Q Ag m

(28)

In a similar way, the dimensionless diagonal linear orbital vibronic coupling constant of the LUMO for the mth Ag mode is defined by Eq. (29),

⎛ 1 ∂h ⎞ ga LUMO (ω m ) = a LUMO ⎜ ⎟ a LUMO ωm ⎝ ∂ qAg m ⎠ 0

(29)


13

D. Vibronic Interactions in Polyfluoroacenes, B, NSubstituted Polyacenes, and Polycyanodienes Similar discussions can be made in the monocations and anions of polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes. The numbers of vibronic active modes are 6, 9, 12, 15, 18, and 21 for 1fa, 2fa, 3fa, 4fa, 5fa, and 6fa, respectively, those are 11, 17, and 23 for 1bn, 2bn, and 3bn, respectively, and those are 5, 7, 9, and 11 for 1cn, 2cn, 3cn, and 4cn, respectively.

Chapter III

ELECTRON–PHONON COUPLING CONSTANTS FOR THE CHARGED ELECTRONIC STATES OF POLYACENES, POLYFLUOROACENES, B, N-SUBSTITUTED POLYACENES, AND POLYCYANODIENES Let us next discuss the total electron–phonon coupling constants ( ltotal ) in the monocation and monoanion crystals. Since the ltotal is the sum of the electron– phonon coupling constants originating from both intramolecular vibrations ( lintra ) and intermolecular vibrations ( linter ), the ltotal is defined as ltotal = lintra + linter .

(30)

However, it should be noted that the intramolecular orbital interactions are much stronger than the intermolecular orbital interactions. Therefore, it is rational that the lintra values are much larger than the linter values in molecular systems. In fact, it is considered by several researchers that the contribution from the intramolecular modes in molecular systems is decisive in the pairing process in the superconductivity in doped C60. [15,32] For example, it was reported that the lintra values are much larger than the linter values in K3C60 and Rb3C60 ( lintra ≥ 10linter ). [32] Furthermore, it has also been shown from a neutronscattering investigation [33] that the electron–libration intramolecular-mode

Takashi Kato

16

coupling is small in alkali-metal-doped C60. Therefore, we consider only intramolecular electron–phonon coupling in this study. The ltotal value for the charged and excited electronic states can be defined as ltotal ≈ lintra = l LUMO (for the electronic state of the monoanion),

(31) = lHOMO (for the electronic state of the monocation),

(32) In the previous section, the vibronic interactions in free polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes were discussed. We can derive the ltotal by using the vibronic coupling constants defined in the previous section as follows. As described above, since polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes would consist of strongly bonded molecules arranged on a lattice with weak van der Waals intermolecular bonds, we can derive the dimensionless electron–phonon coupling constant λ in a similar way as in theory in previous research. [15,25,27– 29] We use a standard expression for λ , [15,25,27–29] λ=

2 2 1 ∑ ∑ 2 hk,k′ (m,q ) δ (Ek )δ (E k′ ) N( 0) m,q k,k′ 2ω m,q

,

(33)

where ω m,q is the vibrational frequency for the mth phonon mode of wave vector q ; hk, k′ is the corresponding electron–phonon matrix element between the electronic states of wave vectors k and k ′ ; Ek and Ek′ are the corresponding energies measured from the Fermi level (original point in Figure 1 (b)) of polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes; N (0) is the total density of states (DOS) at the Fermi level per spin. The charged electronic states in polyacenes, polyfluoroacenes, B, Nsubstituted polyacenes, and polycyanodienes are essentially composed of the charged electronic states at the equilibrium structures of the ground states in polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes and we can write in the form of Bloch sum: ψ (k ) =

1 ∑ c(k)e ikRφ R N R

(34)

Electron-Phonon Coupling Constants…

17

where R denotes the cell position; N is the number of molecules in the crystal; φ R is wave function which denotes the charged electronic states at the equilibrium structures of the ground state of polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes at the cell position R . If we neglect the intermolecular electron–lattice coupling, hk, k ′ can be reduced to =

hk, k ′ (m,q) = ψ (k )h ψ (k′ )

1 i k – k′ R ∑ c *(k )c(k′)e ( ) hR,R (m,q) N R

(35)

where hR, R is the intramolecular coupling matrix and hR, R(m,q) = φ R h φ R

(36)

For the one-phonon mode with wave vector q , this term takes the following form: hR,R(m, q) = (1 /

N )e

iqR

h00 m

(37)

We insert Eq. (37) in Eq. (35) taking the condition k′ = k – q into account to get hkk– q =

1 h00 mc * (k)c (k – q ) N

(38)

We now proceed to calculate λ by inserting Eq. (38) in Eq. (33) considering that ω m ,q is independent of q . We then obtain λ=

(

1 h00mh00m * 2 c * (k )c(k )c * (k – q)c(k – q)δ (Ek )δ Ek–q ∑ ∑ N N(0) k,k–q m 2 ω 2m,q

)

(39) The partial DOS per molecule at the Fermi level of polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes, n(0) can be rewritten as

Takashi Kato

18 n(0) = (1 / N )∑ c * ( k)c (k )δ (Ek )

(40)

k

We can derive Eq. (41) from Eqs. (39) and (40) using n(0) = N (0) / N , λ=

2 1 ∑ 2 h00 m h00 m * n(0 )2 n(0 ) m 2ω m

(41)

where n(0) is now the DOS per spin and per molecule.

A. Twofold Degenerate Electronic States of The Monocations of Monoanions of Benzene, Hexafluorobenzene, and Borazine Here, for example, let us consider twofold degenerate electronic states such as the monocation of benzene, In such a case, we can assume that nνν ′ (0) = 1 n(0 )δ νν ′ , λ 2

takes the form of Eq. (42): λ=

2 n(0 ) h00 m ∑ 4 m ω 2m

(42)

where h00m = hE2 gm ′

(43)

Here hE m ′ is the derivative matrix of the vibronic coupling matrix, hE m , 2g 2g derived by Eq. (45) with respect to the mode amplitude, QE γm , as 2g hE2 gm ′ =

⎡ ⎛ –QE2g ε m QE2 gθ m ⎞ ⎤ ∂ ⎟ = Am ⎜ hE m ⎥ ⎢ Q Q E2g ε m ⎠ ⎦ ∂ QE γ m 2 g ∂ QE2 gγ m ⎣ ⎝ E2g θm 2g

∂

(44)

where ⎛ –QE2 g εm hE2 gm = Am ⎜ Q ⎝ E2 gθ m

QE2 gθ m ⎞ ⎟ QE2 g εm ⎠

(45)

Electron-Phonon Coupling Constants…

19

and Am is the reduced matrix element and is the slope in the original point (i.e., equilibrium structures of the ground states of 1a ( QE εm = QE θ m = 0 )) on the 2g

2g

potential energy surface of the charged electronic state along each vibrational mode (Figure 1 (b)), and is defined as ⎛ ∂h ⎞ Am = e1g HOMO ⎜ ⎟ e1g HOMO ⎝ ∂QE2 g m ⎠ 0

(46)

2 2 , one can rewrite Eq. (42) as Since h00m = 4 Am

λ = n(0 )∑ m

2 Am

ω 2m

(47)

Using Eqs. (15) and (32), and after some simple transformations, we finally get the relation between the nondimensional electron–phonon coupling constant λ , and the intramolecular vibronic coupling constant, ge HOMO (ω m ), as 1g

λ = ∑λm m

, λ m = n(0 )le HOMO (ω m ), 1g

(48)

where le HOMO (ω m ) is the electron–phonon coupling constant defined as 1g le1g HOMO (ω m ) = ge1g HOMO (ω m ) ω m , ( m = 1,2,3,4 ). 2

(49)

In a similar way, the le HOMO (ω m ) for the A1g vibronic active modes can be 1g defined as le1g HOMO (ω m ) =

1 2 ge HOMO (ω m ) ω m 2 1g , ( m = 5,6 ).

(50)

In a similar way, le LUMO (ω m ) for the monoanion of benzene can be defined 2u as le2 u LUMO (ω m ) = ge2u LUMO (ω m ) ω m , ( m = 1,2,3,4 ). 2

(51)

Takashi Kato

20 le2 u LUMO (ω m ) =

1 2 g (ω ) ω m 2 e2 u LUMO m , ( m = 5,6 ).

(52)

Similar discussions can be made in the monocations and monoanions of 1fa and 1bn.

B. Nondegenerate Electronic Systems of Polyacenes, Polyfluoroacenes, B, N-Substituted Polyacenes, and Polycyanodienes In a similar way, by using Eq. (41), the lHOMO (ω m ) and lLUMO (ω m ) for the nondegenerate electronic states in the monocations and monoanions of polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes can be defined as lHOMO (ω m ) = g2HOMO (ω m ) ω m ,

(53)

lLUMO (ω m ) = g2LUMO (ω m ) ω m .

(54)

Chapter IV

OPTIMIZED STRUCTURES A. Benzene and Polyacenes The structures of neutral 1a and polyacenes were optimized under D6h and D2h symmetries, respectively, using the hybrid Hartree–Fock (HF)/density-functionaltheory (DFT) method of Becke [34] and Lee, Yang, and Parr [35] (B3LYP) and the 6-31G* basis set. [36] GAUSSIAN 98 program package [37] was used for our theoretical analyses. This level of theory is, in our experience, sufficient for reasonable descriptions of the geometric, electronic, and vibrational structures of hydrocarbons. An optimized D6h structure of 1a and D2h structures of polyacenes are shown in Figure 2. These structures were confirmed to be a minimum on each potential energy surface from vibrational analyses. We can see that in the D6h structure of 1a there is no bond alternation and all C–C bond lengths are approximately 1.4 Å. In the D2h structure of 2a, there is a distinct variation in the C–C distances. This result can be understood in view of the orbital patterns of the HOMO. Selected vibronic active modes and the phase patterns of the HOMOs and LUMOs of the neutral molecules under consideration are shown in Figure 3. We can see from this figure that the atomic orbitals between two neighboring C2a and C3a atoms are combined in phase and thus form a strong π-bonding in the HOMO of 2a. On the other hand, the HOMO contributes nonbonding interactions between C1a and C1b atoms and between C1a and C2a atoms, and an antibonding interaction between C3a and C3b atoms. This is the reason why the C2a–C3a bond is much shorter (1.377 Å) than any other C–C bond (1.417–1.434 Å). Similar discussions can be made in 3a, 4a, 5a, and 6a; the C–C bond distances between two neighboring carbon atoms whose atomic orbitals are combined in phase (out of phase) are short (long).

Takashi Kato

22

1.397

1a

d7 d8

13 30 . 70 d3 d1 1.4 1.4 00 d2 1.445 1.426

21 1.37 d4 7 1.4 d3 d2 1.417 d5 d4 d1 1.434

d1

2a

d6

d3

d5

d4

d7

1 34 .367 10 1.4 1.4 1. 39 3 d1 1.452 1.451 1.430

4a

3a

1.3 65 d3 d1 .43 .41 1. 40 1 14.3 891 6 2 d2 1.457 1.455 1.433

d6 d4

d5

1 .4 8 .4 7 .366 1.4 017. 991 1 1 8 1 3 .3 7 3 1.460 1.459 1.457 1.434

5a 1.335 d1 1.394

1.338 19 1.37 5 1.4

d3 d2 d4 d1 1.442

d5

d7

d2

d3 d4 d1

d4

1.335 1.410

d3

d5

d1 d2

1.337 1.3 68 1.334 29 1.4 1.418 1.448

1.341 1.4 01

3fa

2fa

1fa

d6

6a

1.339 1.337 1. 3 1.3 94 66 2 33 1.334 1 4 . 4 . 1 1 1.422 1.454 1.452

d7 d8

d6 d4

d3

d5

1.338 1.339 1.338 1.3 1.3 1.4 90 64 05 d1 1.335 16 34 1.4 1.4 d2 1.424 1.456 1.458

4fa 1.0 1 N

B

0

1.200 1.431

1bn 1.3 55

5fa 1.194 6 11.195 .4 2 4 7 1.4 1.4 1.012 42 1.461 1.433 4 1.44 3 4 0 1.197 1. 26 1.4 1.014 1.021

41 1.012 1.4 1. 1.196 42 6 1.433 1.460 1.011 1.4 8 45 1.42 1.197

3bn

2bn

1 61 .316 1.3

1.088 1.355

1cn

1.430

1 .3

74 1.3 1.446

1.089 1.424

2cn 1 49 .325 1.3

1.456

36

1.3

06

1.090 1.437

3cn 1.3

79 1.3 1.457

02

1.090 1.445

4cn

Figure 2. Optimized structures of the neutral polyacenes, polyfluoroacenes, B, Nsubstituted polyacenes, and polycyanodienes.


23

B. Polyfluoroacenes Hexafluorobenzene (C6F6) (1fa) has been well studied for a long time. [38– 53] 1a and 1fa have nearly the same polarizations and polarizability anisotropies. [50] As well as being similar in molecular geometry and shape, 1a and 1fa have similar physical properties. [51] Their electric quadruple moments are roughly equal in magnitude but opposite in sign. [52,53] In recent review, [54] the study of Jahn–Teller and pseudo-Jahn–Teller effects in various molecular systems including the monoanion [55] and cation [56,57] of 1fa are well summarized. The structures of neutral 1fa was optimized under D6h symmetry, and 2fa, 3fa, 4fa, and 5fa were optimized under D2h symmetry. According to our calculations, the energy differences between the HOMO and LUMO of 1fa, 2fa, 3fa, 4fa, and 5fa are 6.52, 4.56, 3.35, 2.57, and 2.03 eV, respectively, and those of 1a, 2a, 3a, 4a, and 5a are 6.80, 4.83, 3.59, 2.78, and 2.21 eV, respectively. Therefore, the HOMO–LUMO gaps in polyfluoroacenes are slightly smaller than those in polyacenes. This can be understood in view of the orbital patterns of the HOMO and LUMO in these molecules. We can see from Figure 3 that the phase patterns of the LUMO of polyfluoroacenes are not significantly different from those of polyacenes. The phase patterns of the LUMO in carbon framework of polyfluoroacenes are similar to those of polyacenes in that the LUMO of polyfluoroacenes is rather localized on carbon framework and the electron density on fluorine atoms is low, and the LUMO of polyacenes is completely localized on carbon atoms. The phase patterns of the HOMO in carbon framework of polyfluoroacenes are also similar to those of polyacenes. However, the HOMO of polyfluoroacenes is delocalized and the electron density on fluorine atoms is not small, while the HOMO of polyacenes is completely localized on carbon atoms. The atomic orbitals between two neighboring carbon and fluorine atoms are combined out of phase in the HOMO in polyfluoroacenes. Therefore, the HOMO is slightly destabilized in energy measured from the LUMO in polyfluoroacenes by H–F substitution. This is the reason why the energy difference between the HOMO and LUMO in polyfluoroacenes is slightly smaller than that in polyacenes. Let us look into optimized structures of polyfluoroacenes. We can see from Figure 2 that the calculated C–C distances in 1fa are 1.394 Å. There is a distinct variation in the C–C distances in polyfluoroacenes. This result is reasonable in view of the HOMOs.The C–C distances between two neighboring carbon atoms whose atomic orbitals are combined in phase (out

Takashi Kato

24 C(1)

HOMO (a)

C(2) C(10)C(1) C(9) C(3)

C(2)

C(8) C(4) C(7) C(6)C(5) LUMO 2a F(18) F(11) C(10) C(2)F(12) F(17) C(9) C(1) C(3) C(4) C(8) F(16)C(7) C(6) C(5)F(13) F(15)F(14) LUMO (a) LUMO (b) LUMO HOMO 1fa B(1 2fa B(10)N(1B(2) N(2) N(9) ) N(3) N(6) ) B(8) B(4) B(5)N(4)B(3) N(7)B(6) N(5) LUMO (a) LUMO (b) LUMO 2bn HOMO 1bn

C(3) C(4) HOMO (b) LUMO (a) LUMO (b) 1a HOMO

HOMO (a) HOMO (b)

HOMO (a) HOMO (b)

C(1) N(2) C(3) C(4) HOMO

1021 cm–1

567 cm–1

LUMO

1cn

–1 1656 cm–1 1a 521 cm

–1

1530 cm–1 1687 cm–1 1271 cm 1fa

1399 cm–1

1035 cm–1

1713 cm–1 1cn

LUMO

HOMO

555 cm–1

–1 2a 1417 cm–1 1630 cm

1402 cm–1

1492 cm–1 1bn

2cn

1552 cm–1

1666 cm–1 2fa

1486 cm–1 2bn

1436 cm–1

1597 cm–1 2cn

Figure 3. The phase patterns of the HOMO and LUMO and selected vibronic active modes in polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes.


25

of phase) in the HOMOs of polyfluoroacenes are short (long). It should be noted that the C–C distances in polyfluoroacenes are similar to those in polyacenes; most of the C–C bond lengths differences between polyacenes and polyfluoroacenes are smaller than 0.003 Å. Only the d4 value difference between 2a and 2fa, d5 value difference between 3a and 3fa, d7 value difference between 4a and 4fa, and d8 value difference between 5a and 5fa are somewhat large (0.007–0.009 Å). Therefore, carbon framework structures in polyfluoroacenes are not significantly different from those in polyacenes as a consequence of H–F substitution.

C. B, N-Substituted Polyacenes Substitution of carbon with boron and nitrogen have been carried out, producing totally substituted boron nitride nanotubes (BN-NTs). [58] Many researchers have studied and compared the structure of these new boron–nitrogencontaining fullerenes and nanotubes with that of carbon nanotubes (C-NTs). [59– 73] A large number of molecular boron–nitrogen compounds have been prepared. [74–79] Because borazine (B3N3H6) (1bn) is both isoelectronic and isosteric with 1a, it is a very interesting compound. Stock and Pohland [80] first reported formation of borazine 1bn from the thermolysis (200 ˚C) of the addition complex [H2B(NH2)2+][BH4–], [81] formulated in 1926 as B2N6·2NH3. Laubengayer and coworkers [82] studied the gas-phase pyrolysis of 1bn in greater detail, and they proposed the intermediate formation of a naphthalene analogue, B5N5H8 (2bn). The structure of neutral “inorganic benzene”, B3N3H6 (1bn) was optimized under D3h symmetry, and “inorganic-” naphthalene (B5N5H8) (2bn) and anthracene (B7N7H10) (3bn) were optimized under C2v symmetry. According to our calculations, the energy difference between the HOMO and the LUMO of 1bn (8.27 eV) is larger than that of 1a (6.80 eV). Furthermore, that of 2bn (7.12 eV) is larger than that of 2a (4.83 eV), and that of 3bn (6.68 eV) is larger than that of 3a (3.59 eV). This can be understood as follows. The degenerate 1a levels have not been split apart in energy but the HOMO contains more nitrogen character than boron character while opposite is true for the LUMO.[30] This is a result clearly in keeping with an electronegativity perturbation on 1a. [30] Due to the electronegativity perturbation, the HOMO (LUMO) of 1bn is stabilized (destabilized) in energy with respect to the HOMO (LUMO) of 1a. This is the reason why the HOMO–LUMO gap is larger in 1bn than in 1a. Similar discussions can be made in 2bn and 3bn. Let us next look into optimized structure of 1bn. We can see from Figure 2 that

26

Takashi Kato

the calculated B–N, B–H, and N–H distances in 1bn are 1.431, 1.200, and 1.010 Å, respectively, and those determined from experimental method [83] are 1.44, 1.20, and 1.02 Å, respectively. Therefore, the structure optimized at the B3LYP/6-31G* level of theory is in excellent agreement with that determined from the experimental method. There is a distinct variation in the B–N distances in 2bn and 3bn. This result is reasonable in view of the HOMOs shown in Figure 3. The B–N distances between two neighboring B and N atoms whose atomic orbitals are combined in phase (out of phase) in the HOMOs of 2bn and 3bn are short (long). It should be noted that the B–N distance (1.431 Å) in 1bn is larger than the C–C distance (1.397 Å) in 1a, but smaller than the B–N single bond distance (1.60 Å). Therefore, it can be said that each B–N bond in 1bn acquires double bond character. Similar discussion can be made in 2bn and 3bn; all B–N bonds in 2bn and 3bn are longer than all C–C bonds in 2a and 3a, but smaller than 1.6 Å.

D. Polycyanodienes We can expect that in the monocations of polycyanodienes, the electron– phonon interactions become much stronger than in the monocations of polyacenes because the strong σ-orbital interactions as well as the π-orbital interactions between two neighboring atoms in the HOMO are significant, [84] and because the HOMO is delocalized and the electron density on hydrogen atoms as well as on carbon and nitrogen atoms is high in the HOMO of polycyanodienes. We call this system “σ-conjugated momocations”. The structures of polycyanodienes were optimized under D2h symmetry. According to our calculations, the energy differences between the HOMO and LUMO of 1cn, 2cn, 3cn, and 4cn are 5.16, 3.97, 3.19, and 2.68 eV, respectively. Therefore, the HOMO–LUMO gaps in polycyanodienes are slightly smaller than those in polyacenes.

Chapter V

ELECTRON–PHONON COUPLING CONSTANTS A. The Monocations and Monoanions of Benzene and Polyacenes We next carried out vibrational analyses of 1a and polyacenes at the B3LYP/6-31G* level. Agreement with experiment is excellent for the vibrational frequencies, calculated wave numbers of 1a being accurate within a range of 2.5–4 %. Since the conventional Hartree–Fock method overestimates molecular vibrational frequencies by typically 10 %, this hybrid DFT method appears to be very useful for vibrational analyses. We next calculated first-order derivatives at this equilibrium structure on each orbital energy surface by distorting the molecule along the A1g and E2g modes of 1a and the Ag modes of polyacenes. In these calculations, the step size of the normal-mode displacements was taken to be in the order of 10–1. What we obtained from the first-order derivatives are the dimensionless diagonal linear orbital vibronic coupling constants gHOMO (ω m ) and gLUMO (ω m ). We can estimate the electron–phonon coupling constants lHOMO (ω m ) and lLUMO (ω m ) from the dimensionless diagonal linear orbital vibronic coupling constants by using Eqs. (49)–(54). The calculated electron–phonon coupling constants in the monocatins and anions of 1a and polyacenes are shown in Figures 4 and 5, respectively. Let us next take a look at the electron–phonon coupling of the A1g and E2g vibrational modes to the e1g HOMO in 1a. E2g modes of 1a are classified into a C–C–C in-plane bending (622 cm–1), a C–H in-plane bending (1208 cm–1), a C–C stretching (1656 cm–1), and a C–H stretching (3184 cm–1). Figure 4

28

Takashi Kato

demonstrates that the E2g vibrational modes of 622 and 1656 cm–1 strongly couple to the e1g HOMO in 1a. This can be understood in view of the orbital patterns of the e2u LUMO and vibrational modes of 1a. When 1a is distorted along this E2g mode toward the direction as shown in Figure 3, the antibonding (bonding) interactions between C1b and C1c in the HOMO (a) (HOMO (b)) become strong, and the bonding interactions between C1a and C1b and between C1c and C1d in the HOMO (a) become weak. Therefore, the HOMO (a) (HOMO (b)) is significantly destabilized (stabilized) in energy. On the other hand, when 1a is distorted toward the opposite direction along the arrow of this mode, the HOMO (a) (HOMO (b)) is significantly stabilized (destabilized) in energy. This is the reason why the E2g mode of 1656 cm–1 strongly couples to the e1g HOMO in 1a. Figure 4 demonstrates that the C–C stretching Ag modes of 1417 and 1630 cm–1 strongly couple to the HOMO in 2a. When 2a is distorted along the Ag mode of 1417 cm–1 toward the direction as shown in Figure 3, the antibonding interactions between C3a and C3b in the HOMO become strong, and the bonding interactions between C2a and C3a and between C2b and C3b become weak. Therefore, the HOMO of 2a is significantly destabilized in energy. On the other hand, when 2a is distorted toward the opposite direction, the HOMO is significantly stabilized in energy. This is the reason why the C–C stretching Ag mode of 1417 cm–1 strongly couples to the HOMO. In a similar way, the C–C stretching Ag mode of 1630 cm–1 strongly couples to the HOMO. In the two frequency modes, the displacements of carbon atoms are very large compared with any other Ag mode of 2a, and the HOMO is completely localized on carbon atoms. It is rational that a frequency mode in which normal displacements are large for atoms where there exists considerable orbital amplitude can strongly couple to the molecular orbital. Identical discussions can be made in 3a, 4a, 5a, and 6a; the C–C stretching Ag modes around 1500 cm–1 and the lowest frequency Ag mode strongly couple to the HOMOs. Let us take a look at the electron–phonon coupling of the A1g and E2g vibrational modes to the e2u LUMO in 1a. We can see from Figure 5 that the E2g mode of 1656 cm–1 strongly couples to the e2u LUMO in 1a. This can be also understood in view of the phase patterns of the e2u LUMO and vibrational modes of 1a. Figure 5 demonstrates that the C–C stretching Ag modes of 1417 and 1630 cm–1 strongly couple to the b1g LUMO. In the two frequency modes, the displacements of carbon atoms are very large compared with any other Ag mode of 2a, and the b1g LUMO is completely localized on carbon atoms. It is rational that a frequency mode in which normal displacements are large for atoms where

Electron-Phonon Coupling Constants 200

1a +

180

Coupling constant (meV)


200 160 140 120 100 80 60 40 20 0

0

500



140 120 100 80 60 40

0

500

1000 1500 2000 2500 3000 3500 Frequency (cm –1)

200

160 140 120 100 80 60 40 20 0

500

4a +

180 160 140 120 100 80 60 40 20 0

1000 1500 2000 2500 3000 3500 Frequency (cm –1)

200

0

500

1000 1500 2000 2500 3000 3500 Frequency (cm –1)

200

5a +

180



160

0

1000 1500 2000 2500 3000 3500 Frequency (cm –1)

3a +

180

160 140 120 100 80 60 40 20 0

2a +

180

20

200

0

29

160 140 120 100 80 60 40 20 0

0

500

1000 1500 2000 2500 3000 3500 Frequency (cm –1)

6a +

180

0

500

1000 1500 2000 2500 3000 3500 Frequency (cm –1)

Figure 4. Electron–phonon coupling constants for the monocations of polyacenes.

there exists considerable orbital amplitude can strongly couple to the molecular orbital. Identical discussions can be made in 3a, 4a, 5a, and 6a; the C–C stretching Ag modes around 1500 cm–1 and the lowest frequency Ag mode strongly couple to the LUMOs. The C–C stretching Ag modes around 1500 cm–1 strongly couple to

Takashi Kato

30

the HOMOs as well as to the LUMOs in polyacenes. But it should be noted that the lowest frequency modes as well as the C–C stretching modes strongly couple to the LUMO in polyacenes, while the only C–C stretching modes strongly couple to the HOMO in polyacenes. 200

1a–

180

160

160

140

140

120

120 100

100

80 60 40 20 0

0

500



160 140 120 100 80 60 40 20 0

500

20 0

500

1000 1500 2000 2500 3000 3500 Frequency (cm –1)

4a–

180 160 140 120 100 80 60 40 20 0

500

1000 1500 2000 2500 3000 3500 Frequency (cm –1)

200

5a–

180



40

0

1000 1500 2000 2500 3000 3500 Frequency (cm –1)

200 160 140 120 100 80 60 40 20 0

60

200

3a–

180

80

0

1000 1500 2000 2500 3000 3500 Frequency (cm –1)

200

0

2a–

180



200

160 140 120 100 80 60 40 20 0

0

500

1000 1500 2000 2500 3000 3500 Frequency (cm –1)

6a–

180

0

500

1000 1500 2000 2500 3000 3500 Frequency (cm –1)

Figure 5. Electron–phonon coupling constants for the monoanions of polyacenes.

Electron-Phonon Coupling Constants

31

B. Polyfluoroacenes 1. Monocations We carried out vibrational analyses of polyfluoroacenes at the B3LYP/631G* level of theory. There are four E2g modes in 1fa (C–C–F in-plane bending mode of 259 cm–1; C–C–C in-plane bending mode of 444 cm–1; C–F stretching mode of 1192 cm–1; C–C stretching mode of 1687 cm–1). There are four E2g vibrational modes in 1a (C–C–C in-plane bending mode of 622 cm–1; C–C–H inplane bending mode of 1208 cm–1; C–C stretching mode of 1656 cm–1; C–H stretching mode of 3184 cm–1). Therefore, the frequencies for the C–C–H in-plane bending mode (1208 cm–1) and for the C–H stretching mode (3184 cm–1) in 1a are much larger than those for the C–C–F in-plane bending mode (259 cm–1) and for the C–F stretching mode (1192 cm–1) in 1fa, respectively, as expected. Furthermore, the frequency for the C–C–C in-plane bending mode (622 cm–1) in 1a is larger than that (444 cm–1) in 1fa. The frequency for the C–C stretching mode (1656 cm–1) in 1a is similar to that (1687 cm–1) in 1fa. The calculated electron–phonon coupling constants in the monocations and monoanions of 1fa, 2fa, 3fa, 4fa, and 5fa are shown in Figures 6 and 7, respectively. We can see from Figure 6 that the C–C stretching E2g mode of 1687 cm–1 can strongly couple to the e1g HOMO in 1fa. This can be understood in view of the phase patterns of the HOMO in 1fa. The reduced mass for the E2g mode of 1687 cm–1 is 12.05, and the displacements of carbon atoms are much larger than those of fluorine atoms in the mode. When 1fa is distorted along the E2g mode of 1687 cm–1 toward the same direction as shown in Figure 3, the antibonding (bonding) interactions between two neighboring carbon atoms in the HOMO (a) (HOMO (b)) become significantly stronger, and the bonding interactions between two neighboring carbon atoms in the HOMO (a) become significantly weaker, and thus the HOMO (a) (HOMO (b)) is significantly destabilized (stabilized) in energy by such a distortion. This is the reason why the E2g mode of 1687 cm–1 the most strongly couples to the e1g HOMO in 1fa.

Takashi Kato

32 250

250

2fa+

200



1fa+

150

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Figure 6. Electron–phonon coupling constants for the monocations of polyfluoroacenes.

We can see from Figure 6 that the A1g mode of 1530 cm–1 can very strongly couple to the e1g HOMO in 1fa. This can be understood as follows. When 1fa is distorted along the A1g mode of 1530 cm–1, the bonding interactions between two neighboring carbon atoms become significantly weaker, and the antibonding interactions between two neighboring carbon and fluorine atoms in the e1g HOMO become significantly stronger, and thus the e1g HOMO is significantly


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Figure 7. Electron–phonon coupling constants for the monoanions of polyfluoroacenes.

destabilized in energy by such a distortion in 1fa. This is the reason why the A1g mode of 1530 cm–1 can strongly couple to the e1g HOMO in 1fa. The A1g mode of 567 cm–1 much less strongly couples to the e1g HOMO than the A1g mode of 1530 cm–1 in 1fa. This can be understood as follows. When 1fa is distorted along the A1g mode of 567 cm–1, the bonding interactions between two neighboring carbon atoms and the antibonding interactions between two neighboring carbon and fluorine atoms in the e1g HOMO become weaker. Since such weakened effects of

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bonding and antibonding interactions are compensated by each other, the e1g HOMO is slightly stabilized in energy by such a distortion in 1fa. This is the reason why the A1g mode of 567 cm–1 much less strongly couples to the e1g HOMO than the A1g mode of 1530 cm–1 in 1fa. We can see from Figure 6 that the C–C stretching Ag mode of 1666 cm–1 the most strongly couples to the HOMO in 2fa. This can be understood as follows. When 2fa is distorted along the Ag mode of 1666 cm–1, the bonding and antibonding interactions between two neighboring carbon atoms become significantly stronger and weaker, respectively, and the antibonding interactions between two neighboring carbon and fluorine atoms in the HOMO in 2fa become weaker. Therefore, the HOMO is significantly stabilized in energy by such a distortion in 2fa. This is the reason why the Ag mode of 1666 cm–1 can the most strongly couple to the HOMO in 2fa. In a similar way, the Ag modes of 514 and 1552 cm–1 also strongly couple to the HOMO in 2fa. Similar discussions can be made in 3fa, 4fa, and 5fa; the low frequency mode around 500 cm–1, the high frequency modes around 1200 cm–1, and the frequency modes around 1600 cm–1 afford large electron–phonon coupling constants in the monocations of polyfluoroacenes.

2. Monoanions Let us first look into the electron–phonon interactions between the E2g modes and the e2u LUMO in 1fa. We can see from this figure that the C–C stretching E2g mode of 1687 cm–1 can strongly couple to the e2u LUMO in 1fa. This can be understood in view of the phase patterns of the LUMO in 1fa. When 1fa is distorted along the E2g mode of 1687 cm–1 toward the same direction as shown in Figure 3, the bonding (antibonding) interactions between two neighboring carbon atoms in the LUMO (a) become stronger (weaker), therefore, the LUMO (a) is significantly stabilized in energy. In a similar way, the antibonding interactions between two neighboring carbon atoms in the LUMO (b) become stronger by such a distortion, therefore, the LUMO (b) is significantly destabilized in energy. This is the reason why the E2g mode of 1687 cm–1 can strongly couple to the e2u LUMO in 1fa. In addition to this mode, the C–F stretching E2g mode of 1192 cm–1 can strongly couple to the e2u LUMO, but the E2g modes of 259 and 444 cm–1 hardly couple to it. This can be understood as follows. The reduced masses for the E2g modes of 1192 and 1687 cm–1 are 13.69 and 12.05, respectively, therefore, the displacements of carbon atoms are much larger than those of fluorine atoms in these modes. On the other


35

hand, the reduced masses for the E2g modes of 259 and 444 cm–1 are 18.62 and 16.08, respectively, and therefore, the displacements of fluorine atoms are more dominant than those of carbon atoms in these modes. Since the e2u LUMO is rather localized on carbon atoms, it is reasonable that a frequency mode in which normal displacements of carbon atoms are large (small), can strongly (weakly) couple to the e2u LUMO. This is the reason why the E2g modes of 1192 and 1687 cm–1 can strongly couple to the e2u LUMO, while the E2g modes of 259 and 444 cm–1 hardly couple to it. Let us next look into the electron–phonon interactions between the A1g modes and the e2u LUMO in 1fa. We can see from Figure 7 that the A1g mode of 567 cm– 1 much more strongly couples to the e2u LUMO than the A1g mode of 1530 cm–1 in 1fa. This can be understood as follows. When 1fa is distorted along the A1g mode of 567 cm–1, the antibonding interactions between two neighboring carbon atoms, and between two neighboring carbon and fluorine atoms, both in the LUMO (a) and LUMO (b), become weaker. Therefore, both the LUMO (a) and LUMO (b) are significantly stabilized in energy by such a distortion. When 1fa is distorted along the A1g mode of 1530 cm–1, the antibonding interactions between two neighboring carbon atoms, and between two neighboring carbon and fluorine atoms, become weaker and stronger, respectively, both in the LUMO (a) and LUMO (b). Since such strengthened and weakened effects of antibonding interactions are compensated by each other, the A1g mode of 1530 cm–1 less strongly couples to the e2u LUMO than the A1g mode of 567 cm–1. Let us next look into the electron–phonon interactions between the Ag modes and the b1g LUMO in 2fa. We can see from Figure 7 that the C–C stretching Ag mode of 1402 cm–1 much more strongly couples to the LUMO than the other modes in 2fa. This can be understood as follows. The reduced mass for the Ag mode of 1402 cm–1 is 12.11, therefore, the displacements of carbon atoms are much larger than those of fluorine atoms in the mode. When 2fa is distorted along the Ag mode of 1402 cm–1, the bonding (antibonding) interactions between two neighboring carbon atoms become stronger (weaker), and the antibonding interactions between two neighboring carbon and fluorine atoms in the LUMO become weaker. Therefore, the LUMO is significantly stabilized in energy by such a distortion. This is the reason why the Ag mode of 1402 cm–1 strongly couples to the LUMO in 2fa. We can see from Figure 7 that the Ag modes of 1271 and 1552 cm–1 also somewhat strongly couple to the LUMO in 2fa. This can be understood as follows. When 2fa is distorted along the Ag mode of 1552 cm–1, the bonding interactions between C(3) and C(4) atoms, and between C(8) and C(9) atoms, become stronger, and the antibonding interactions between C(3) and F(12) atoms, between C(4) and F(13) atoms,

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between C(8) and F(16) atoms, and between C(9) and F(17) atoms, in the LUMO, become weaker. Therefore, the LUMO is stabilized in energy by such a distortion. This is the reason why the Ag mode of 1552 cm–1 also somewhat strongly couples to the LUMO in 2fa. But it should be noted that the antibonding interactions between C(2) and C(3) atoms, between C(4) and C(5) atoms, between C(7) and C(8) atoms, and between C(9) and C(10) atoms in the LUMO, become slightly stronger, and thus the LUMO would be slightly destabilized in energy by such an effect. The destabilization effect and the stabilization effect described above are compensated by each other, the LUMO is slightly stabilized in energy by such a distortion. This is the reason why the Ag mode of 1552 cm–1 much less strongly couples to the LUMO than the Ag mode of 1402 cm–1 even though both Ag modes are C–C stretching modes and the reduced mass for the Ag mode of 1552 cm–1 is similar to that for the Ag mode of 1402 cm–1. When 2fa is distorted along the C–F stretching Ag mode of 1271 cm–1, the antibonding interactions between C(2) and F(11) atoms, between C(5) and F(14) atoms, between C(7) and F(15) atoms, and between C(10) and F(18) atoms in the LUMO, become stronger, therefore, the LUMO is destabilized in energy by such a distortion. But there are not significant changes in the strengths of the orbital interactions between two neighboring carbon atoms in the mode, and thus the C–F stretching Ag mode of 1271 cm–1 much less strongly couples to the LUMO than the C–C stretching Ag mode of 1402 cm–1 in 2fa. Similar discussions can be made in 3fa, 4fa, and 5fa; the C–C stretching Ag modes of 1401, 1389, and 1379 cm–1 the most strongly couple to the LUMO in 3fa, 4fa, and 5fa, respectively. Let us next compare the calculated results in polyfluoroacenes with those in polyacenes. As in case of the monoanion of 1fa, the C–C stretching E2g mode of 1656 cm–1 affords the largest electron–phonon coupling constant (193 meV) in the monoanion of 1a. But it should be noted that the C–C stretching E2g mode of 1687 cm–1 in the monoanion of 1fa affords a larger electron–phonon coupling constant (223 meV) than the C–C stretching E2g mode of 1656 cm–1 in the monoanion of 1a. This can be understood as follows. The reduced mass for the E2g mode of 1656 cm–1 in 1a is 5.32, and therefore, the displacements of hydrogen atoms as well as those of carbon atoms are large in the mode. On the other hand, the reduced mass for the E2g mode of 1687 cm–1 in 1fa is 12.05, and thus, the displacements of carbon atoms are very large and those of fluorine atoms are very small in the mode. The LUMO is completely localized on carbon atoms in 1a, and is rather localized on carbon atoms in 1fa. Therefore, it is rational that the E2g mode of 1687 cm–1 in 1fa in which the displacements of carbon atoms are larger, more strongly couples to the LUMO localized on


37

carbon atoms than the E2g mode of 1656 cm–1 in 1a in which the displacements of carbon atoms are smaller. Similar discussions can be made in 2fa, 3fa, 4fa, and 5fa; the C–C stretching modes afford larger electron–phonon coupling constants in the monoanions of 2fa, 3fa, 4fa, and 5fa than in the monoanions of 2a, 3a, 4a, and 5a, respectively. This is because the displacements of carbon atoms in the modes are larger in 2fa, 3fa, 4fa, and 5fa than those in 2a, 3a, 4a, and 5a, respectively, and the orbital patterns of the LUMO in polyacenes hardly change by H–F substitution. It should be noted that the C–C stretching modes around 1500 cm–1 and the low frequency modes, less and more, respectively, strongly couple to the LUMO with an increase in molecular size in polyacenes, while the low frequency modes as well as the C–C stretching modes around 1500 cm–1 less strongly couple to the LUMO with an increase in molecular size in polyfluoroacenes. It should be noted that the A1g mode of 567 cm–1 (1530 cm–1) much more (less) strongly couples to the e2u LUMO than to the e1g HOMO in 1fa. This can be understood as follows. When 1fa is distorted along the A1g mode of 567 cm–1, the antibonding interactions between two neighboring carbon atoms and between two neighboring carbon and fluorine atoms in the e2u LUMO in 1fa become significantly weaker, and thus the e2u LUMO is significantly stabilized in energy, while the energy level of the e1g HOMO does not significantly change by such a distortion because the weakened effects of bonding and antibonding interactions are compensated by each other, as described above. This is the reason why the A1g mode of 567 cm–1 much more strongly couples to the e2u LUMO than to the e1g HOMO in 1fa. When 1fa is distorted along the A1g mode of 1530 cm–1, the antibonding interactions between two neighboring carbon atoms and between two neighboring carbon and fluorine atoms in the e2u LUMO in 1fa become weaker and stronger, respectively. Since such weakened and strengthened effects of antibonding interactions are compensated by each other, the e2u LUMO in 1fa is slightly destabilized in energy by such a distortion. On the other hand, such a compensation does not occur in the electron–phonon interactions between the e1g HOMO and the A1g mode of 1530 cm–1, as described above. This is the reason why the A1g mode of 1530 cm–1 much more strongly couples to the e1g HOMO than to the e2u LUMO in 1fa. But it should be noted that the high frequency E2g modes of 1192 and 1687 cm–1 (the low frequency E2g modes of 259 and 444 cm–1) much more (less) strongly couple to the e2u LUMO than to the e1g HOMO in 1fa. This can be understood as follows. The reduced masses for the high frequency E2g modes of 1192 and 1687 cm–1 are 13.69 and 12.05, respectively, and thus the displacements of carbon atoms are much larger than those of fluorine atoms in these modes in 1fa, while those

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Takashi Kato

for the low frequency E2g modes of 259 and 444 cm–1 are 18.62 and 16.08, respectively, and thus the displacements of fluorine atoms are larger than those of carbon atoms in these modes in 1fa. The e2u LUMO is rather localized on carbon atoms and in which the electron density on fluorine atoms are low, on the other hand, the e1g HOMO is delocalized and in which the electron density on fluorine atoms are as high as those on carbon atoms in 1fa. It is rational that the higher (lower) frequency E2g modes, in which the displacements of carbon (fluorine) atoms are very large, more (less) strongly couple to the e2u LUMO rather localized on carbon atoms than to the delocalized e1g HOMO in 1fa. This is the reason why the high frequency E2g modes of 1192 and 1687 cm–1 (the low frequency E2g modes of 259 and 444 cm–1) much more (less) strongly couple to the e2u LUMO than to the e1g HOMO in 1fa. It should be noted that the Ag mode of 1666 cm–1 (1402 cm–1) much more (less) strongly couples to the HOMO than to the LUMO in 2fa. This can be understood as follows. When 2fa is distorted along the Ag mode of 1666 cm–1, the bonding and antibonding interactions between two neighboring carbon atoms in the LUMO in 2fa become weaker and stronger, respectively, and thus the LUMO would be destabilized in energy by such a distortion. On the other hand, the antibonding interactions between two neighboring carbon and fluorine atoms in the LUMO in 2fa become weaker, and thus the LUMO would be stabilized in energy by such a distortion. Since such destabilization and stabilization effects are compensated by each other, the LUMO is slightly destabilized in energy by such a distortion in 2fa. Such a compensation does not occur in the electron–phonon interactions between the Ag mode of 1666 cm–1 and the HOMO in 2fa, and thus the Ag mode of 1666 cm–1 much more strongly couples to the HOMO than to the LUMO in 2fa. In a similar way, such a compensation occurs (does not occur) in the electron–phonon interactions between the Ag mode of 1402 cm–1 and the HOMO (LUMO), and thus the energy level of the LUMO much more significantly changes than that of the HOMO by such a distortion in 2fa. This is the reason why the Ag mode of 1402 cm–1 can much more strongly couple to the LUMO than to the HOMO in 2fa. That is, the significant phase patterns difference between the HOMO, in which the atomic orbitals between two neighboring carbon atoms are mainly combined in phase and those between two neighboring carbon and fluorine atoms are combined out of phase, and the LUMO, in which the atomic orbitals between two neighboring carbon atoms and between two neighboring carbon and fluorine atoms are combined out of phase, is the main reason why the vibrational modes which play an essential role in the electron–phonon


39

interactions in the monocations are significantly different from those in the monoanions in 2fa. In a similar way, we can rationalize in view of the phase patterns of the HOMO and LUMO the calculated results that the frequency modes lower than 500 cm–1 and the high frequency modes around 1400 cm–1 much more strongly couple to the LUMO than to the HOMO in 2fa, 3fa, 4fa, and 5fa, on the other hand, the frequency modes around 500 cm–1 and the frequency modes around 1600 cm–1 much more strongly couple to the HOMO than to the LUMO in 2fa, 3fa, 4fa, and 5fa.

C. B, N-Substituted Polyacenes 1. Monocations There are five kinds of E´ vibrational modes in 1bn (B–N–B or N–B–N inplane bending mode of 520 cm–1; B–N–H or N–B–H in-plane bending modes of 951 and 1073 cm–1; B–N stretching modes of 1399 and 1492 cm–1; B–H stretching mode of 2625 cm–1; N–H stretching mode of 3640 cm–1). The frequencies of the vibrational modes in B, N-substituted polyacene-series are slightly lower than those in polyacene-series. For example, the frequencies of the B–N stretching modes of 1399 and 1492 cm–1 in 1bn are lower than that of the C– C stretching mode of 1656 cm–1 in 1a. This can be understood as follows. The B– N bonds in 1bn are longer than the C–C bonds in 1a. In general, the frequency of the stretching mode between two neighboring atoms whose bond lengths are larger, is lower. The C–H (1.087 Å) bond lengths in 1a lie between the N–H (1.010 Å) and B–H (1.200 Å) bond lengths in 1bn, and the frequency for the C–H (3184 cm–1) stretching mode in 1a also lies between those for the N–H (3640 cm– 1 ) and B–H (2625 cm–1) stretching modes in 1bn. The calculated electron–phonon coupling constants in the monocations and monoanions of 1bn, 2bn, and 3bn are shown in Figure 8. We can see from Figure 3 that the HOMO and LUMO in B, N-substituted polyacene-series are rather localized on N and B atoms, respectively, due to the electronegativity perturbation on polyacene-series. We can see from Figure 8 that the B–N stretching E´ mode of 1492 cm–1 can strongly couple to the e´ HOMO in 1bn. This can be understood in view of phase patterns of the HOMO in 1bn. When 1bn is distorted along the E´ mode of 1492 cm–1 toward the same direction as shown in Figure 3, the bonding (antibonding) interactions between two neighboring B and N atoms in the HOMO (a) become stronger (weaker), therefore, the HOMO (a) is significantly

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stabilized in energy. In a similar way, the bonding interactions between two neighboring B and N atoms in the HOMO (b) become weaker by such a distortion, therefore, the HOMO (b) is significantly destabilized in energy. This is the reason why the E´ mode of 1492 cm–1 can strongly couple to the e´ HOMO in 1bn. In addition to this mode, the E´ modes of 520 and 1399 cm–1 and the A1´ mode of 949 cm–1 can also couple to the e´ HOMO in 1bn. But it should be noted that the E´ mode of 1399 cm–1 much less strongly couples to the e´ HOMO than the E´ mode of 1492 cm–1 even though both vibrational modes are the B–N stretching modes. This can be understood as follows. The reduced mass for the E´ mode of 1399 cm–1 is 1.89, while that for the E´ mode of 1492 cm–1 is 4.93, and thus the displacements of B and N atoms are larger in the E´ mode of 1492 cm–1 than in the E´ mode of 1399 cm–1. The e´ HOMO is, on the other hand, localized on B and N atoms. It is rational that a frequency mode in which the displacements of B and N atoms are important, more strongly couples to the e´ HOMO localized on B and N atoms. This is the reason why the E´ mode of 1399 cm–1 much less strongly couples to the e´ HOMO than the E´ mode of 1492 cm–1 in 1bn. It should be noted that the B–H stretching E´ mode of 2636 cm–1 somewhat couples to the e´ HOMO in 1bn. Considering that the electron density on boron and hydrogen atoms in the e´ HOMO is not high, such electron–phonon coupling constant for the E´ mode of 2636 cm–1 is rather large. Let us next look into the electron–phonon coupling in the monocations of 2bn and 3bn. We can see from Figure 8 that the B–N stretching A1 mode of 1486 cm–1 can strongly couple to the HOMO in 2bn. Furthermore, the B–N stretching A1 modes of 1480 and 1528 cm–1 strongly couple to the HOMO in 3bn. It should be noted that the electron–phonon coupling constants for the low frequency modes decrease with an increase in molecular size from the monocations of 1bn to 3bn more rapidly than those for the B–N stretching modes around 1500 cm–1. Let us next compare the calculated results for the monocations of B, Nsubstituted polyacenes with those for the monocations of polyacenes. We can see from Figure 8 that as in the monocation of 1bn, both the low frequency modes and the C–C stretching modes around 1500 cm–1 afford large electron–phonon coupling constants in the monocation of 1a. But in the monocations of large size of polyacenes such as 2a and 3a, only the C–C stretching modes around 1500 cm– 1 afford large electron–phonon coupling constants, and the electron–phonon coupling constants for the C–C stretching modes around 1500 cm–1 decrease with an increase in molecular size from the monocations of 2a to 6a.




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Figure 8. Electron–phonon coupling constants for the monocations and monoanions of B, N-substituted polyacenes.

2. Monoanions We can see from Figure 8 that the B–N stretching E´ mode of 1492 cm–1 can strongly couple to the e´ LUMO in 1bn. This can be understood in view of the phase patterns of the LUMO in 1bn. When 1bn is distorted by the E´ mode of

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1492 cm–1 toward the same direction as shown in Figure 3, the bonding (antibonding) interactions between two neighboring B and N atoms in the LUMO (a) become weaker (stronger), therefore, the LUMO (a) is significantly destabilized in energy. In a similar way, the antibonding interactions between two neighboring B and N atoms in the LUMO (b) become weaker by such a distortion, therefore, the LUMO (b) is significantly stabilized in energy. That is the reason why the E´ mode of 1492 cm–1 can strongly couple to the e´ LUMO in 1bn. In addition to this mode, the E´ mode of 1073 cm–1 and the A1´ mode of 949 cm–1 can also couple to the e´ LUMO in 1bn. But it should be noted that the B–N stretching E´ mode of 1399 cm–1 hardly couples to the e´ LUMO in 1bn. This can be understood as follows. When 1bn is distorted by the E´ mode of 1399 cm–1 toward the same direction as shown in Figure 3, the bonding (antibonding) interaction between N(1) and B(2) becomes stronger, while the bonding (antibonding) interaction between B(3) and N(3) becomes weaker in the LUMO (a) (LUMO (b)). Since such changes in the strengths of orbital interactions are compensated by each other, the energy levels of the LUMO (a) and LUMO (b) are not significantly changed by such a distortion. That is the reason why the B–N stretching E´ mode of 1399 cm–1 hardly couples to the e´ LUMO in 1bn. Let us next look into the electron–phonon coupling in the monoanions of 2bn and 3bn. We can see from Figure 8 that the lowest frequency A1 modes of 327 and 447 cm– 1 and the B–N stretching mode of 1486 cm–1 can strongly couple to the a2 LUMO in 2bn. Furthermore, the lowest frequency A1 modes of 212 and 345 cm–1 and the B–N stretching A1 mode of 1480 cm–1 can strongly couple to the b1 LUMO in 3bn. It should be noted that the B–N stretching modes around 1500 cm–1 and the low frequency modes, less and more, respectively, strongly couple to the LUMO with an increase in molecular size from 1bn to 3bn. Let us next compare the calculated results for the monocations with those for the monoanions [74] in B, N-substituted polyacenes. As described above, the HOMO and LUMO in B, N-substituted polyacene-series are rather localized on N and B atoms, respectively, due to the electronegativity perturbation on polyaceneseries. Therefore, significant vibronic interactions character differences between the monoanions and cations in B, N-substituted polyacene-series can be expected. As can be seen from Figure 8, both the low frequency modes and the B–N stretching modes around 1500 cm–1 afford large electron–phonon coupling constants in the monoanions and cations in B, N-substituted polyacenes. The low frequency modes play more important role in the electron–phonon interactions in the monocation than in the monoanion in 1bn. But the electron–phonon coupling constants for the low frequency modes decrease more rapidly with an increase in molecular size than those for the B–N stretching modes around 1500 cm–1 in the


43

monocations of B, N-substituted polyacene-series. Therefore, the B–N stretching modes would play more important role in the electron–phonon interactions than the low frequency modes even in the large size of the monocations of B, Nsubstituted polyacenes. But the B–N stretching modes around 1500 cm–1 and the low frequency modes, less and more, respectively, strongly couple to the LUMO with an increase in molecular size from 1bn to 3bn. Therefore, the higher frequency modes would play an essential role in the electron–phonon interactions in the large size of the monocations, while the lower frequency modes play such a role in the large size of the monoanions in B, N-substituted polyacenes. This difference may come from the phase patterns difference between the HOMO and LUMO due to electronegativity perturbation on polyacene-series. We can therefore conclude in this section that the lower frequency modes play an important role in the electron–phonon interactions in large size of the negatively charged polyacene-series and B, N-substituted polyacene-series, while the higher frequency modes such as B–N stretching modes around 1500 cm–1 play such a role in the positively charged polyacene-series and B, N-substituted polyacene-series.

D. Polycyanodienes 1. Monocations The calculated electron–phonon coupling constants in the monocations of 2cn, 3cn, and 4cn are shown in Figure 9. Let us next look into the electron– phonon interactions between the ag HOMO and the Ag modes in 2cn. We can see from Figure 9 that the Ag mode of 1597 cm–1 the most strongly couples to the ag HOMO in 2cn. This can be understood in view of the phase patterns of the HOMO in 2cn. When 2cn is distorted along the Ag mode of 1597 cm–1 toward the same direction as shown in Figure 3, the bonding interactions between C(3) and C(4) atoms in the HOMO become weaker, and the antibonding interactions between N(2) and C(3) atoms become stronger. Furthermore, the characteristics of the bonding and antibonding interactions between two neighboring carbon and hydrogen atoms in the HOMO become less and more, respectively, significant. Therefore, the ag HOMO is significantly destabilized in energy by such a distortion. This is the reason why the Ag mode of 1597 cm–1 the most strongly couples to the ag HOMO in 2cn. In addition to this, the lowest frequency Ag mode of 555 cm–1 affords large electron–phonon coupling constant in the monocation of 2cn. When 2cn is distorted along the Ag mode of 555 cm–1, the characteristics of

Takashi Kato

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the antibonding interactions between N(2) and C(3) atoms become more significant, and the bonding interactions between two neighboring carbon and hydrogen atoms in the HOMO become weaker. Therefore, the ag HOMO is significantly destabilized in energy by such a distortion. This is the reason why the Ag mode of 555 cm–1 affords large electron–phonon coupling constant in the monocation of 2cn. Similar discussions can be made in 3cn and 4cn; the C–C and C–N stretching modes around 1500 cm–1 and the lowest frequency modes strongly couple to the HOMO. 300

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Figure 9. Electron–phonon coupling constants for the monocations of polycyanodienes.

2. Monoanions The calculated electron–phonon coupling constants in the monoanions of 1cn, 2cn, 3cn, and 4cn are shown in Figure 10. Let us first look into the electron– phonon interactions between the Ag modes and the b3u LUMO in 1cn. We can see from Figure 10 that the Ag mode of 1713 cm–1 can the most strongly couple to the


45

b3u LUMO in 1cn. When 1cn is distorted along the Ag mode of 1713 cm–1 toward the same direction as shown in Figure 3, the bonding interactions between two neighboring carbon atoms in the b3u LUMO become stronger, and the antibonding interactions between two neighboring carbon and nitrogen atoms become weaker, and thus the b3u LUMO is significantly stabilized in energy. This is the reason why the Ag mode of 1713 cm–1 can the most strongly couple to the b3u LUMO in 1cn. The Ag mode of 1035 cm–1 also strongly couples to the b3u LUMO in 1cn. When 1cn is distorted along the Ag mode of 1035 cm–1, the antibonding interactions between two neighboring carbon and nitrogen atoms in the b3u LUMO become significantly weaker, and thus the b3u LUMO is significantly stabilized in energy by such a distortion. On the other hand, the bonding interactions between two neighboring carbon atoms become also slightly weaker by such a distortion, the b3u LUMO would be slightly destabilized in energy. Such stabilized and destabilized effects are compensated by each other. Therefore, the Ag mode of 1035 cm–1 affords slightly smaller electron–phonon coupling constant than the Ag mode of 1713 cm–1 in the monoanion of 1cn. Furthermore, the Ag mode of 623 cm–1 also somewhat strongly couples to the b3u LUMO in 1cn. The reduced masses for the Ag modes of 623, 1035 and 1713 cm–1 are large, and are 8.80, 7.53 and 5.97, respectively, in 1cn. Therefore, the displacements of carbon and nitrogen are large in these modes. It is rational that the Ag modes of 623, 1035, and 1713 cm–1, in which the displacements of carbon and nitrogen atoms are larger, can strongly couple to the b3u LUMO localized on carbon and nitrogen atoms. On the other hand, the reduced masses for the Ag modes of 1252 and 3200 cm–1 are 1.11 and 1.10, respectively. It is rational that the Ag modes of 1252 and 3200 cm–1 in which the displacements of carbon and nitrogen atoms are small cannot strongly couple to the b3u LUMO localized on carbon and nitrogen atoms. This is the reason why the Ag modes of 623, 1035, and 1713 cm–1 can more strongly couple to the b3u LUMO than the Ag modes of 1252 and 3200 cm–1 in 1cn. Let us look into the electron–phonon interactions between the Ag modes and the b1g LUMO in 2cn. We can see from Figure 10 that the Ag mode of 1597 cm–1 strongly couples to the b1g LUMO in 2cn. This can be understood as follows. When 2cn is distorted along the Ag mode of 1597 cm–1, the bonding interactions between two neighboring carbon atoms in the b1g LUMO become significantly weaker, and the antibonding interactions between two neighboring carbon and nitrogen atoms become significantly stronger, and thus the b1g LUMO is significantly destabilized in energy by such a distortion in 2cn. This is the reason why the Ag mode of 1597 cm–1 can strongly couple to the b1g LUMO in 2cn. The Ag mode of 1436 cm–1 can also strongly couple to the b1g LUMO in

Takashi Kato

46

2cn. When 2cn is distorted along the Ag mode of 1436 cm–1, the antibonding interactions between two neighboring carbon and nitrogen atoms in the b1g LUMO in 2cn become stronger, and thus the b1g LUMO is significantly destabilized in energy by such a distortion in 2cn. 200

160 140 120 100 80 60 40 20 0

500

1000 1500 2000 2500 Frequency (cm –1 )

3000

140 120 100 80 60 40

0

3500

0

500

1000

1500

2000

Frequency (cm

200

–1

2500

3000

3500

2500

3000

3500

)

200

3cn–

180

4cn–

180

160



160

20

0

140 120 100 80 60 40 20 0

2cn–

180 Coupling constant (meV)


200

1cn–

180

160 140 120 100 80 60 40 20

0

500

1000

1500

2000

Frequency (cm

–1

2500 )

3000

3500

0

0

500

1000

1500

2000

Frequency (cm

–1

)

Figure 10. Electron–phonon coupling constants for the monoanions of polycyanodienes.

This is the reason why the Ag mode of 1436 cm–1 strongly couples to the b1g LUMO in 2cn. Apart from the C–H stretching Ag mode of 3187 cm–1, the electron–phonon coupling constant increases with an increase in frequency in 2cn. In the low frequency modes, which have similar characteristics to those of acoustic mode of phonon in solids, all atoms move toward the similar direction. Therefore, the orbital interactions between two neighboring atoms do not significantly change when 2cn is distorted along the low frequency Ag modes. This is the reason why the electron–phonon coupling decreases with a decrease in frequency in 2cn. The C–H stretching mode of 3187 cm–1 hardly couples to the b1g LUMO in 2cn. The reduced mass for the Ag mode of 3187 cm–1 is 1.10,


47

and in which the displacements of carbon and nitrogen atoms are very small. The b1g LUMO is localized on carbon and nitrogen atoms in 2cn. It is rational that the Ag mode of 3187 cm–1, in which the displacements of carbon and nitrogen atoms are very small, hardly couples to the b1g LUMO localized on carbon and nitrogen atoms in 2cn. Similar discussions can be made in the monoanions of 3cn and 4cn; the C–C stretching modes around 1500 cm–1 can strongly couple to the LUMO.

E. Summary In this chapter, we investigated the electron–phonon interactions in the monocations and monoanions of polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes. The C–C stretching modes around 1500 cm–1 strongly couple to the HOMO, and the lowest frequency modes and the C–C stretching modes around 1500 cm–1 strongly couple to the LUMO in polyacenes. The C–C stretching modes around 1500 cm–1 strongly couple to the HOMO and LUMO in polyfluoroacenes. The B–N stretching modes around 1500 cm–1 strongly couple to the HOMO and LUMO in B, N-substituted polyacenes. The C– C and C–N stretching modes around 1500 cm–1 strongly couple to the HOMO and LUMO in polycyanodienes.

Chapter VI

TOTAL ELECTRON–PHONON COUPLING CONSTANTS A. Polyacenes and Polyfluoroacenes 1. Monocations Let us next discuss the total electron–phonon coupling constants in the monocations ( lHOMO ) of polyfluoroacenes, and compare the calculated results for polyfluoroacenes with those for polyacenes. The lHOMO values for 1a and 1fa are defined as

lHOMO =

6

∑ lHOMO(ω m ) =

m=1

4

6

1 2 (ω m ) ω m + ∑ g2HOMO(ω m ) ω m ∑ gHOMO 2 m=5 m=1 (55)

and those for polyacenes and polyfluoroacenes (2fa–5fa and 2fa–5fa) are defined as 2 lHOMO = ∑ lHOMO (ω m ) = ∑ gHOMO (ω m ) ω m m

m

(56)

The calculated total electron–phonon coupling constants ( lLUMO and lHOMO ) in the monoanions and cations of polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes are shown in Figure 11. The lHOMO values are

50

Takashi Kato

estimated to be 0.418, 0.399, 0.301, 0.255, and 0.222 eV for 1fa, 2fa, 3fa, 4fa, and 5fa, respectively, and those are estimated to be 0.244, 0.173, 0.130, 0.107, and 0.094 eV for 1a, 2a, 3a, 4a, and 5a, respectively. Therefore, the lHOMO values decrease with an increase in molecular size in both polyacenes and polyfluoroacenes. This can be understood as follows. The electron density per atom in the HOMO becomes lower with an increase in molecular size, and the orbital interactions between two adjacent atoms become weaker with an increase in number of atoms in polyacenes and polyfluoroacenes. Therefore, strengths of the orbital interactions between two adjacent atoms less significantly change with an increase in number of atoms when these monocations are distorted along the C–C stretching modes around 1500 cm–1 playing an essential role in the electron– phonon interactions. This is the reason why the lHOMO value decreases with an increase in number of atoms. Therefore, in general, we can expect that a monocation, in which number of carriers per atom is larger, affords larger lHOMO value. The lHOMO values for polyfluoroacenes are much larger than those for polyacenes. This can be understood as follows. For example, let us compare the calculated results for 2fa with those for 2a. The reduced masses of the C–C stretching Ag modes of 1445 and 1610 cm–1 in 2a, which afford large electron– phonon coupling constants in the monocation of 2a, are 9.68 and 7.19, respectively, and thus the displacements of carbon atoms are not very large in these vibrational modes. On the other hand, the reduced masses of the C–C stretching modes of 1552 and 1666 cm–1 in 2fa, which afford large electron– phonon coupling constants in the monocation of 2fa, are 12.45 and 12.10, respectively, and thus the displacements of carbon atoms are very large in these vibrational modes. It is rational that the C–C stretching modes around 1500 cm–1, in which the displacements of carbon atoms are larger in 2fa, can more strongly couple to the HOMO, in which the electron density on carbon atoms are very high, than the C–C stretching modes around 1500 cm–1, in which the displacements of carbon atoms are smaller in 2a. Furthermore, the low frequency mode of 514 cm–1 affords much larger electron–phonon coupling constant in the monocation of 2fa than the low frequency modes around 500 cm–1 in the monocation of 2a. Similar discussion can be made in 3fa, 4fa, and 5fa. Therefore, we can conclude that the larger values of the electron–phonon coupling constants for the C–C stretching modes around 1500 cm–1 in the monocations of polyfluoroacenes than those in the monocations of polyacenes due to the larger displacements of carbon atoms in the C–C stretching modes in polyfluoroacenes than those in polyacenes, and the larger values of the electron–

Total Electron-Phonon Coupling Constants

51

phonon coupling constants for the low frequency modes around 500 cm–1 in the monocations of polyfluoroacenes than those in the monocations of polyacenes, are the main reason why the lHOMO values for polyfluoroacenes are much larger than

Electron–phonon coupling constants (eV)

those for polyacenes. 0.6 0.5 0.4 0.3 0.2 0.1 0.0

0

5

10

15

20

25

Number of B, C, and N atoms Figure 11. Total electron–phonon coupling constants for the monocations and monoanions of polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes. The opened circles, triangles, squares, and diamonds represent the lHOMO values for polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes, respectively, and the closed circles, triangles, squares, and diamonds represent the lLUMO values for polyacenes, polyfluoroacenes, polycyanodienes, respectively.

B,

N-substituted

polyacenes,

and

2. Monoanions Let us next discuss the total electron–phonon coupling constants in the monoanions ( lLUMO ) of polyfluoroacenes, and compare the calculated results for polyfluoroacenes with those for polyacenes. The lLUMO value for 1fa is defined as

Takashi Kato

52 lLUMO =

6

4

m=1

m=1

1

6

2 (ω m ) ω m + ∑ g2LUMO(ω m ) ω m ∑ lLUMO(ω m ) = ∑ gLUMO 2 m=5

(57)

and that for polyfluoroacenes (2fa–5fa) is defined as 2 lLUMO = ∑ lLUMO (ω m ) = ∑ gLUMO (ω m ) ω m m

m

(58)

The lLUMO values are estimated to be 0.475, 0.473, 0.350, 0.273, and 0.215 eV for 1fa, 2fa, 3fa, 4fa, and 5fa, respectively, while those are estimated to be 0.322, 0.255, 0.186, 0.154, and 0.127 eV for 1a, 2a, 3a, 4a, and 5a, respectively. Therefore, the lLUMO values decrease with an increase in molecular size in both polyacenes and polyfluoroacenes. The lLUMO values for polyfluoroacenes are much larger than those for polyacenes. This can be understood as follows. As described above, the LUMOs of polyfluoroacenes are rather localized on carbon atoms, and those of polyacenes are completely localized on carbon atoms. And the displacements of carbon atoms in the C–C stretching modes around 1500 cm–1 in polyfluoroacenes become larger than those in polyacenes as a consequence of H–F substitution in polyacenes. That is, by substituting hydrogen atoms by heavier atoms which have the highest electronegativity in every element, fluorine atoms, the displacements of carbon atoms become significantly larger in the C–C stretching modes, while the electronic structure in the LUMO hardly changes. Therefore, the C–C stretching modes around 1500 cm–1 in polyfluoroacenes more strongly couple to the LUMO localized on carbon atoms than those in polyacenes. This is the main reason why the lLUMO values for polyfluoroacenes are much larger than those for polyacenes. The lLUMO value for polyfluoroacenes decreases with an increase in molecular size more rapidly than that for polyacenes, and the lLUMO values difference between polyacenes and polyfluoroacenes decreases with an increase in molecular size. This is because the ratio of the number of fluorine atoms to that of carbon atoms becomes smaller from 1fa to 5fa, and the effects of H–F substitution become less important in this order. Let us next compare the calculated results for the monocations with those for the monoanions in polyfluoroacenes. The lLUMO values are larger than the lHOMO values in 1fa, 2fa, 3fa, and 4fa. This can be understood as follows. The C–C stretching modes around 1500 cm–1, in which the displacements of carbon atoms are very large, can more strongly couples to the LUMO rather localized on carbon


53

atoms than to the delocalized HOMO in polyfluoroacenes. This is the reason why the electron–phonon coupling constants for the C–C stretching Ag modes around 1400 cm–1 in the monoanions are larger than those for the C–C stretching Ag modes around 1600 cm–1 in the monocations in polyfluoroacenes, and the reason why the lLUMO values are larger than the lHOMO values in 1fa, 2fa, 3fa, and 4fa. But it should be noted that the lLUMO value decreases with an increase in molecular size more rapidly than the lHOMO value in polyfluoroacenes, and the lLUMO value is slightly smaller than the lHOMO value in 5fa. The lHOMO and lLUMO values for polyfluoroacene with D2h geometry would converge and be estimated by extrapolation in Figure 11 to be 0.074 and 0.009 eV, respectively, assuming that the lHOMO and lLUMO values are approximately inversely proportional to the number of carbon atoms in each series. The lHOMO value is estimated to be much larger than the lLUMO value in polyfluoroacene ( N → ∞ ), even though the lHOMO value is smaller than the lLUMO value in small size of polyfluoroacenes such as 2fa, 3fa, and 4fa. That is, the lHOMO values decrease with an increase in molecular size less rapidly than the lLUMO values in polyfluoroacenes. This is because the electron–phonon coupling

constants originating from the C–C stretching modes around 1500 cm–1 decrease with an increase in molecular size more rapidly in the monoanions than in the monocations in polyfluoroacenes. The strengths of the orbital interactions between two neighboring carbon atoms in the HOMO and LUMO significantly change when polyfluoroacenes are distorted along the C–C stretching modes around 1500 cm–1, and thus the C–C stretching modes around 1500 cm–1 can strongly couple to the HOMO and LUMO in polyfluoroacenes. Strengths of such orbital interactions in the HOMO become weaker with an increase in molecular size less rapidly than those in the LUMO in polyfluoroacenes because the electron density on carbon atoms in the LUMO rather localized on carbon atoms decrease with an increase in molecular size more rapidly than those in the delocalized HOMO in polyfluoroacenes. This is the reason why the electron–phonon coupling constants originating from the C–C stretching modes around 1500 cm–1 decrease with an increase in molecular size more rapidly in the monoanions than in the monocations in polyfluoroacenes, and the reason why the lHOMO values decrease with an increase in molecular size less rapidly than the lLUMO values in polyfluoroacenes. The total electron–phonon coupling constants were estimated to be 0.322, 0.254, 0.186, 0.154, 0.127, and 0.106 eV (0.244, 0.173, 0.130, 0.107, 0.094, and

Takashi Kato

54

0.079 eV) in the monoanions (monocations) of 1a, 2a, 3a, 4a, 5a, and 6a, respectively. Therefore, the electron–phonon coupling constants decrease with an increase in molecular size. Figures 4 and 5 demonstrate that the electron–phonon coupling originating from the C–C stretching modes of 1400–1600 cm–1 becomes weaker as the molecular size becomes larger from 1a to 6a. Thus, the C–C stretching modes should play an important role in the electron–phonon coupling in the monoanions and cations of 1a and polyacenes. The total electron–phonon coupling constants in the monocations of polyacenes ( lHOMO ) are smaller than those in the monoanions ( lLUMO ). This is because the lowest frequency mode, which plays an important role in the electron–phonon coupling in the monoanions of polyacenes, does not play a role in the electron–phonon coupling in the monocations.

B. B, N-Substituted Polyacenes The lHOMO for 1bn is defined as 11

7

m=1

m=1

2 lHOMO = ∑ lHOMO (ω m ) = ∑ gHOMO (ω m ) ω m +

1 11 2 ∑ gHOMO (ω m ) ω m 2 m=8

(59)

That for 2bn is defined as 17

17

m =1

m =1

2 lHOMO = ∑ lHOMO (ω m ) = ∑ gHOMO (ω m ) ω m

(60)

and that for 3bn is defined as 23

23

m =1

m =1

2 lHOMO = ∑ lHOMO (ω m ) = ∑ gHOMO (ω m ) ω m

(61)

The lLUMO for 1bn is defined as

lLUMO =

11

7

m =1

m =1

1 11

2 2 (ω m ) ω m + ∑ gLUMO (ω m ) ω m ∑ lLUMO(ω m ) = ∑ gLUMO 2 m =8

(62)


55

That for 2bn is defined as lLUMO =

17

17

m =1

m =1

2 (ω m ) ω m ∑ lLUMO(ω m ) = ∑ gLUMO

(63)

and that for 3bn is defined as lLUMO =

23

23

m =1

m =1

2 (ω m ) ω m ∑ lLUMO(ω m ) = ∑ gLUMO

(64)

The lHOMO ( lLUMO ) values are estimated to be 0.357, 0.209, and 0.182 eV (0.340, 0.237, and 0.203 eV) for 1bn, 2bn, and 3bn, respectively, while those are estimated to be 0.244, 0.173, and 0.130 eV (0.322, 0.254, and 0.186 eV) for 1a, 2a, and 3a, respectively. Therefore, both the lHOMO and lLUMO values decrease with an increase in molecular size in B, N-substituted polyacene-series as well as in polyacene-series. The lLUMO values are much larger than the lHOMO values in polyacene-series, while the lHOMO values are similar to the lLUMO values in B, N-substituted polyacene-series. This can be understood as follows. The low frequency modes as well as the C–C stretching modes around 1500 cm–1 afford electron–phonon coupling constants in the monoanions of polyacenes, while only the C–C stretching modes around 1500 cm–1 afford large electron–phonon coupling constants in the monocations of polyacenes except for 1a. Furthermore, the C–C stretching modes around 1500 cm–1 and the low frequency modes, less and more, respectively, strongly couple to the LUMO, while the C–C stretching modes around 1500 cm–1 less strongly couple to the HOMO with an increase in molecular size in polyacene-series. The electron–phonon coupling originating from the low frequency modes in the monoanions is the main reason why the lLUMO values are much larger than the lHOMO values in polyacene-series. Let us next look into B, N-substituted polyacene-series. The B–N stretching modes around 1500 cm–1 as well as the low frequency modes afford large electron– phonon coupling constants both in the monoanions and cations of B, Nsubstituted polyacene-series. The B–N stretching modes around 1500 cm–1 and the low frequency modes, less and more, respectively, strongly couple to the LUMO with an increase in molecular size, while the low frequency modes much less strongly couple to the HOMO than the B–N stretching modes around 1500 cm–1 with an increase in molecular size in B, N-substituted polyacene-series. Even

56

Takashi Kato

though the low and high frequency modes afford large electron–phonon coupling constants in the monoanions and cations in B, N-substituted polyacene-series, respectively, there are not significant differences between the lLUMO and lHOMO values. This is the reason why the lLUMO values are similar to the lHOMO values in B, N-substituted polyacene-series. We can see from Figure 11 that the lHOMO values for B, N-substituted polyacenes are larger than those for polyacenes, and can expect that those for the large size of B, N-substituted polyacene-series are larger than those for the large size of polyacene-series. The lHOMO values for B, N-substituted polyacene ( N → ∞ ) and polyacene ( N → ∞ ) are estimated to be 0.096 and 0.036 eV, respectively, assuming that the lHOMO is approximately inversely proportional to the number of C, B, and N atoms in each series.65 This can be understood as follows. For example, let us compare the HOMO of 3bn with that of 3a. We can see from Figure 3 that the HOMO of 3a is rather localized on C(1), C(3), C(5), C(8), C(10) and C(12) atoms which are located at the edge of the carbon framework, and the electron density on other carbon atoms is very low. Therefore, the HOMO of 3a has a non-bonding character and the orbital interactions between two neighboring carbon atoms are not so large. Such a non-bonding character in the HOMO becomes more significant with an increase in molecular size in polyacene-series. This is the reason why the lHOMO values decrease with an increase in molecular size in polyacene-series. Let us next look into 3bn. Because of the electronegativity perturbation on 3a, the HOMO of 3bn is stabilized in energy with respect to the HOMO of 3a, and the electron density on N(7), N(9), N(11), and N(13) atoms in 3bn is higher than that on C(7), C(9), C(11), and C(13) atoms in 3a, respectively. Therefore, orbital interactions between N(7) and B(8), between B(8) and N(9), between N(9) and B(10), between B(10) and N(11), between N(11) and B(12), and between B(12) and N(13) atoms in the HOMO of 3bn, are stronger than those between two neighboring carbon atoms in the HOMO of 3a. This is the reason why the lHOMO value for 3bn is larger than that for 3a. In a similar way, the large size of B, N-substituted polyacene-series would have larger lHOMO values than the large size of polyacene-series. We can therefore conclude that because of the strong orbital interactions between B and N atoms in the HOMO in B, N-substituted polyacene-series as a consequence of the electronegativity perturbation on polyacene-series, the lHOMO values for B, Nsubstituted polyacene-series would become larger than those for polyacene-series.


57

C. Polycyanodienes 1. Monocations Let us next discuss the total electron–phonon coupling constants in the monocations ( lHOMO ) of polycyanodienes, and compare the calculated results for polycyanodienes

with

those

for

polyacenes.

The

lHOMO

values

for

polycyanodienes are defined as lHOMO = ∑ lHOMO (ω m ) = ∑ gHOMO (ω m ) ω m 2

m

m

(65)

The lHOMO values are estimated to be 0.558, 0.464, and 0.378 eV for 2cn, 3cn, and 4cn, respectively. Those were estimated to be 0.173, 0.130, and 0.107 eV for 2a, 3a, and 4a, respectively. Therefore, the lHOMO values decrease with an increase in molecular size in the monocations of polycyanodienes as well as in the monocations of polyacenes. The lHOMO values for polycyanodienes are much larger than those for polyacenes. This can be understood as follows. The HOMO of polyacenes is localized on edge part of carbon atoms, and thus the nonbonding characteristics are significant in the HOMO of polyacenes. Therefore, the energy levels of the HOMO in polyacenes do not significantly change even if polyacenes are distorted along the C–C stretching modes around 1500 cm–1 playing an essential role in the electron–phonon interactions. As in case of the HOMO of polyacenes, the HOMO of polycyanodienes are also somewhat localized on edge part of nitrogen atoms. On the other hand, the σ orbital interactions as well as the π orbital interactions are significant in the HOMO of polycyanodienes. Therefore, orbital interactions between two neighboring atoms are much stronger in the HOMO of polycyanodienes than in the HOMO of polyacenes. Furthermore, while the HOMO of polyacenes are completely localized on carbon atoms, the HOMO of polycyanodienes are delocalized, and the electron density on hydrogen atoms as well as that on carbon and nitrogen atoms in the HOMO of polycyanodienes is high. Therefore, the strengths of the orbital interactions between two neighboring carbon and hydrogen atoms are significantly changed by distortions by vibronic active modes. This is the reason why the lHOMO values for σ-conjugated polycyanodienes are much larger than those for π-conjugated polyacenes. In summary, the strong σ orbital interactions between two neighboring carbon atoms and two neighboring carbon and nitrogen atoms and the orbital interactions

Takashi Kato

58

between two neighboring carbon and hydrogen atoms in the HOMO of polycyanodienes are the main reason why the lHOMO values for σ-conjugated polycyanodienes are much larger than those for π-conjugated polyacenes. Let us next estimate the lHOMO values for polycyanodienes ( N → ∞ ) with D2h geometry. Assuming that the lHOMO values for polycyanodienes with D2h geometry are approximately inversely proportional to the number of carbon and nitrogen atoms in each series, as suggested in previous research, [21] the lHOMO value for polycyanodiene ( N → ∞ ) is estimated to be 0.167 eV. The lHOMO value for polyacene ( N → ∞ ) with D2h geometry is estimated to be 0.027 eV. Therefore, the lHOMO values for polycyanodienes ( N → ∞ ) are estimated to be much larger than those for polyacenes ( N → ∞ ). Strong σ orbital interactions between two neighboring atoms and the orbital interactions between two neighboring carbon and hydrogen atoms in the HOMO of polycyanodienes are the main reason why the lHOMO values for σ-conjugated polycyanodienes are much larger than those for π-conjugated polyacenes.

2. Monoanions Let us next discuss the total electron–phonon coupling constants in the monoanions ( lLUMO ) of polycyanodienes, and compare the calculated results for polycyanodienes

with

those

for

polyacenes.

The

lLUMO

values

for

polycyanodienes are defined as lLUMO = ∑ lLUMO (ω m ) = ∑ g2LUMO (ω m ) ω m m

m

,

(66)

The lLUMO values are estimated to be 0.478, 0.338, 0.275, and 0.240 eV for 1cn, 2cn, 3cn, and 4cn, respectively, while those are estimated to be 0.322, 0.255, 0.186, and 0.154 eV for 1a, 2a, 3a, and 4a, respectively, and those are estimated to be 0.340, 0.237, and 0.203 eV for 1bn, 2bn, and 3bn, respectively. Therefore, the lLUMO values decrease with an increase in molecular size in polyacenes, B, Nsubstituted polyacenes, and polycyanodienes. The lLUMO values for polycyanodienes are much larger than those for polyacenes. This can be understood in view of the phase patterns of the LUMO in polyacenes and polycyanodienes. The LUMOs of polyacenes are rather localized


59

on carbon atoms located at the edge part of carbon framework. Therefore, nonbonding characteristic is significant in the LUMOs in polyacenes. On the other hand, the LUMO of polycyanodienes is delocalized, and the electron density on carbon atoms as well as on nitrogen atoms located at the edge part of CN framework is high in the LUMO in polycyanodienes. Therefore, the orbital interactions between two neighboring atoms in the LUMO in polycyanodienes are stronger than those in the LUMO in polyacenes. This is the reason why the lLUMO values for polycyanodienes are much larger than those for polyacenes. Let us next discuss why the LUMOs of polyacenes are rather localized on carbon atoms located at the edge part of carbon framework, while those of polycyanodienes are delocalized, and the electron density on carbon atoms as well as on nitrogen atoms is high in the LUMO in polycyanodienes. In general, due to electronegativity perturbation, [30] the π bonding orbitals are weighted more heavily on the atoms which are more electronegative, and the π antibonding orbitals weighted more heavily on the atoms which is less electronegative. As described above, the LUMO are rather localized on carbon atoms which are located at the edge part of carbon framework in polyacenes. In polycyanodienes, carbon atoms with high electron density in the LUMO, located at the edge part of carbon framework of polyacenes, are substituted by nitrogen atoms with the higher electronegativity. Therefore, the electron density on nitrogen atoms in the LUMO in polycyanodienes is lower than that on carbon atoms located at the edge part of carbon framework in the LUMO of polyacenes, and the electron density on carbon atoms which are not located at the edge part of CN framework in the LUMO in polycyanodienes is higher than that on carbon atoms which are not located at the edge part of carbon framework in the LUMO in polyacenes. This is the reason why the LUMOs of polyacenes are rather localized on carbon atoms located at the edge part of carbon framework, while those of polycyanodienes are delocalized, and the electron density on carbon atoms as well as on nitrogen atoms is high in polycyanodienes. Let us next estimate the lLUMO values for polycyanodienes ( N → ∞ ) with D2h geometry. Assuming that the lLUMO values for polycyanodienes with D2h geometry are approximately inversely proportional to the number of carbon and nitrogen atoms in each series, as suggested before, the lLUMO value for polycyanodiene ( N → ∞ ) is estimated to be 0.122 eV. The lLUMO value for polyacene ( N → ∞ ) with D2h geometry was estimated to be 0.019 eV. In summary, the lLUMO values for polycyanodienes are estimated to be much larger than those for polyacenes. Therefore, the orbital patterns difference

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between the LUMO localized on carbon atoms located at the edge part of carbon framework in polyacenes and the delocalized LUMO in polycyanodienes due to electronegativity perturbation, is the main reason why the lLUMO values for polycyanodienes are much larger than those for polyacenes with D2h geometry.

D. Summary In this chapter, we estimated the total electron–phonon coupling constants in the monocations and monoanions of polyacenes, polyfluoroacenes, B, Nsubstituted polyacenes, and polycyanodienes. The lHOMO and lLUMO values decrease with an increase in molecular size in polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes. Electron density per atom in the HOMO becomes lower with an increase in molecular size, and the orbital interactions between two adjacent atoms become weaker with an increase in number of atoms in polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes. Therefore, strengths of the orbital interactions between two adjacent atoms less significantly change with an increase in number of atoms when the monocations and monoanions are distorted along the C–C stretching modes around 1500 cm–1 playing an essential role in the electron–phonon interactions. This is the reason why the lHOMO value decreases with an increase in number of atoms. Therefore, in general, we can expect that monocations and monoanions, in which number of carriers per atom is larger, affords larger lHOMO value. The lHOMO and lLUMO values for polyfluoroacenes are larger than those for polyacenes. Larger values of the electron–phonon coupling constants for the C–C stretching modes around 1500 cm–1 in the monocations and monoanions of polyfluoroacenes than those in the monocations and monoanions of polyacenes due to the larger displacements of carbon atoms in the C–C stretching modes in polyfluoroacenes than those in polyacenes, are main reason why the lHOMO and lLUMO values for polyfluoroacenes are much larger than those for polyacenes. The lHOMO values for B, N-substituted polyacenes are larger than those for polyacenes.

The lLUMO values for B, N-substituted polyacenes are similar to those for polyacenes. The lLUMO values are larger than the lHOMO values in polyacenes, polyfluoroacenes, and B, N-substituted polyacenes. Therefore, electron doping rather than hole doping is more effective way to seek for large electron–phonon coupling constants in polyacenes, polyfluoroacenes, and B, N-substituted polyacenes. Both the lHOMO and lLUMO values for polycyanodienes are larger than


61

those for polyacenes. Therefore, CH–CF, CC–BN, and CC–CN atomic substitutions are effective way to seek for large lHOMO and lLUMO values in polyacenes. The orbital patterns difference between the LUMO localized on carbon atoms located at the edge part of carbon framework in polyacenes and the delocalized LUMO in polycyanodienes due to electronegativity perturbation, is the main reason why the lLUMO values for polycyanodienes are much larger than those for polyacenes. Strong σ orbital interactions between two neighboring carbon atoms and two neighboring carbon and nitrogen atoms and the orbital interactions between two neighboring carbon and hydrogen atoms in the HOMO of polycyanodienes are the main reason why the lHOMO values for σ-conjugated polycyanodienes are much larger than those for π-conjugated polyacenes. The lHOMO values are larger than the lLUMO values in polycyanodienes. Strong σ orbital interactions between two neighboring carbon atoms and two neighboring carbon and nitrogen atoms and the orbital interactions between two neighboring carbon and hydrogen atoms in the HOMO and the weak π orbital interactions between two neighboring carbon atoms and two neighboring carbon and nitrogen atoms in the LUMO of polycyanodienes, are the main reason why the lHOMO values are larger than the lLUMO values in polycyanodienes.

Chapter VII

THE LOGARITHMICALLY AVERAGED PHONON FREQUENCIES Let us next look into the logarithmically averaged phonon frequencies ω ln for the monocations ( ω ln,HOMO ) and monoanions ( ω ln,LUMO ) of polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes which measure the frequency of the vibrational modes which play an important role in the electron–phonon interactions. The ω ln,HOMO values are defined by lHOMO (ω m )ln ω m ⎫ ⎬ lHOMO ⎭ ⎩m

⎧

ω ln,HOMO = exp ⎨∑

(67)

and the ω ln,LUMO values are defined by lLUMO (ω m )ln ω m ⎫ ⎬ lLUMO ⎭ ⎩m

⎧

ω ln,LUMO = exp ⎨∑

(68)

The logarithmically averaged phonon frequencies for the monoanions ( ω ln,LUMO ) and cations of polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes as a function of molecular weight Mw are shown in Figure 12.

Takashi Kato

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A. Polyacenes and Polyfluoroacenes 1. Monocations The ω ln,HOMO values are estimated to be 1060, 1303, 1341, 1305, and 1270 cm for 1fa, 2fa, 3fa, 4fa, and 5fa, respectively, and those are estimated to be 1164, 1521, 1501, 1450, and 1359 cm–1 for 1a, 2a, 3a, 4a, and 5a, respectively. Therefore, the ω ln,HOMO values decrease with an increase in molecular size in –1

polyacenes (from 2a to 5a) and polyfluoroacenes (from 2fa to 5fa). This is in qualitatively agreement with a tendency in conventional superconductors; light masses will lead to higher values of ω ln . 1600 1400

1000 800

200

–1

)

ω

400

(cm

600

ln

Phonon frequencies

1200

0 0

100

200 300 400 500 Molecular weights Mw

600

Figure 12. Logarithmically averaged phonon frequencies versus molecular weights in the monocations and monoanions of polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes. The opened circles, triangles, squares, and diamonds represent the ω ln,HOMO values for polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes, respectively, and the closed circles, triangles, squares, and diamonds represent the ω ln,LUMO values for polyacenes, polyfluoroacenes, B, Nsubstituted polyacenes, and polycyanodienes, respectively.


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The ω ln,HOMO values for polyfluoroacenes become smaller than those for polyacenes by H–F substitution in polyacenes. This can be understood as follows. The frequencies of the vibronic active modes in polyfluoroacenes are much smaller than those in polyacenes, as expected. Furthermore, the low frequency mode around 500 cm–1 as well as the C–C stretching modes around 1500 cm–1 can strongly couple to the HOMO in polyfluoroacenes, while only the C–C stretching modes around 1500 cm–1 can strongly couple to the HOMO in polyacenes. This is the reason why the ω ln,HOMO values for polyacenes are larger than those for polyfluoroacenes.

2. Monoanions Let us next look into the logarithmically averaged phonon frequencies ω ln for the monoanions of polyfluoroacenes. The ω ln,LUMO values are estimated to be 1112, 1070, 1005, 972, and 1003 cm–1 for 1fa, 2fa, 3fa, 4fa, and 5fa, respectively, and those are estimated to be 1390, 1212, 1023, 926, and 869 cm–1 for 1a, 2a, 3a, 4a, and 5a, respectively. Therefore, the ω ln,LUMO values for polyacenes and polyfluoroacenes decrease with an increase in molecular size. This is in qualitatively agreement with a tendency in conventional superconductors; light mass will lead to higher values of ω ln . But it should be noted that the ω ln,LUMO values for polyfluoroacenes decrease with an increase in molecular size less rapidly than those for polyacenes. This can be understood as follows. In the monoanions of polyacenes, the high frequency modes and the low frequency modes, less and more, respectively, strongly couple to the LUMO with an increase in molecular size, and thus, the ω ln,LUMO values significantly decrease with an increase in molecular size. In the monoanions of polyfluoroacenes, on the other hand, the low frequency modes as well as the high frequency modes less strongly couple to the LUMO with an increase in molecular size, and thus, the ω ln,LUMO values slightly decrease with an increase in molecular size. The ω ln,LUMO values for 1fa, 2fa, and 3fa become smaller than those for 1a, 2a, and 3a,

respectively, by H–F substitution in polyacenes. However, considering the large Mw values difference between 1fa ( Mw = 186 ) and 1a ( Mw = 78 ), between 2fa ( Mw = 272 ) and 2a ( Mw = 128 ), and between 3fa ( Mw = 358 ) and 3a ( Mw = 178 ), the ω ln,LUMO values difference between polyacenes and polyfluoroacenes is not large.

This can be understood as follows. Even though the frequencies of all vibronic

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active modes in polyfluoroacenes are much smaller than those in polyacenes, the displacements of hydrogen and fluorine atoms do not play an essential role in the electron–phonon interactions in the monoanions of polyacenes and polyfluoroacenes, respectively, because the LUMOs are localized on carbon atoms and the electron density on hydrogen and fluorine atoms are very small in polyacenes and polyfluoroacenes, respectively. This is the reason why the ω ln,LUMO values difference between polyacenes and polyfluoroacenes is not large even though the Mw values difference between them is large. Furthermore, the ω ln,LUMO values for 4fa and 5fa are larger than those for 4a and 5a even though the Mw values for 4fa ( Mw = 444 ) and 5fa ( Mw = 530 ) are much larger than those for 4a ( Mw = 228 ) and 5a ( Mw = 278 ), respectively. This is because the low frequency modes as well as the C–C stretching modes around 1500 cm–1 strongly couple to the LUMO in 4a and 5a, while the C–C stretching modes around 1500 cm–1 much more strongly couple to the LUMO than the low frequency modes in 4fa and 5fa. We can expect that in the hydrocarbon molecular systems, the ω ln values would basically decrease by substituting hydrogen atoms by heavier atoms. This can be understood from the fact that the frequencies of all vibronic active modes in polyacenes downshift by H–F substitution. However, considering that the ω ln value for the LUMO rather localized on carbon atoms in 4fa and 5fa becomes larger by H–F substitution, we can expect that the ω ln value for a molecular orbital localized on carbon atoms has a possibility to increase by substituting hydrogen atoms by heavier atoms if the orbital patterns of the molecular orbital do not significantly change by such substitution. Therefore, the detailed properties of the vibrational modes and the electronic structures as well as the molecular weights are closely related to the frequencies of the vibrational modes which play an important role in the electron–phonon interactions in the monoanions of polyfluoroacenes. The ω ln,HOMO values are larger than the ω ln,LUMO values in polyfluoroacenes. This can be understood as follows. The frequency modes lower than 500 cm–1 and the high frequency modes around 1400 cm–1 much more strongly couple to the LUMO than to the HOMO in 2fa, 3fa, 4fa, and 5fa, while the frequency modes around 500 cm–1 and the frequency modes around 1600 cm–1 much more strongly couple to the HOMO than to the LUMO in 2fa, 3fa, 4fa, and 5fa. In particular, the C–C stretching modes around 1600 cm–1 the most strongly couple to the HOMO, while the C–C stretching modes around 1400 cm–1 the most strongly couple to the


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LUMO in 2fa, 3fa, 4fa, and 5fa. This is the reason why the ω ln,HOMO values are larger than the ω ln,LUMO values in polyfluoroacenes. As described above, the significant phase patterns difference between the HOMO and the LUMO is the main reason why the vibrational modes which play an essential role in the electron–phonon interactions in the monocations are significantly different from those in the monoanions in 2fa, 3fa, 4fa, and 5fa. Therefore, the detailed properties of the vibrational modes and the electronic structures as well as the molecular weights are closely related to the frequencies of the vibrational modes which play an important role in the electron–phonon interactions in charged polyfluoroacenes.

B. B, N-Substituted Polyacenes The ω ln,HOMO ( ω ln,LUMO ) values are estimated to be 1154, 1268, and 1337 cm (1273, 737, and 449 cm–1) for 1bn, 2bn, and 3bn, respectively. Therefore, the ω ln,HOMO and ω ln,LUMO values, increase and significantly decrease, respectively, –1

with an increase in molecular size from 1bn to 3bn. As in polyacene-series, the ω ln,HOMO values are larger than the ω ln,LUMO values in large size of B, Nsubstituted polyacene-series. And as in 1a, the ω ln,LUMO value is slightly larger than the ω ln,HOMO value in 1bn. Let us next compare the calculated results for B, N-substituted polyaceneseries with those for polyacene-series. The differences between the ω ln,HOMO and ω ln,LUMO values become larger with an increase in molecular size in B, N-

substituted polyacene-series, while those in polyacene-series hardly change. This can be understood as follows. Let us first look into polyacene-series. [64] The C– C stretching modes around 1500 cm–1 and the low frequency modes strongly couple to the LUMO, and less and more, respectively, strongly couple to the LUMO with an increase in molecular size in polyacene-series. On the other hand, the C–C stretching modes around 1500 cm–1 strongly couple to the HOMO, and less strongly couple to the HOMO with an increase in molecular size in polyacene-series. Therefore, both the ω ln,LUMO and ω ln,HOMO values decrease with an increase in molecular size, and the difference between the ω ln,HOMO and ω ln,LUMO values hardly changes in polyacene-series. Let us next look into B, Nsubstituted polyacene-series. The B–N stretching modes around 1500 cm–1 and

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the low frequency modes strongly couple to the LUMO, and less and more, respectively, strongly couple to the LUMO with an increase in molecular size in B, N-substituted polyacene-series. On the other hand, the B–N stretching modes around 1500 cm–1 and the low frequency modes strongly couple to the HOMO, and the low frequency modes much less strongly couple to the HOMO than the B–N stretching modes around 1500 cm–1 with an increase in molecular size in B, N-substituted polyacene-series. This is the reason why the ω ln,HOMO and ω ln,LUMO values, increase and significantly decrease, respectively, with an increase in molecular size from 1bn to 3bn, and the reason why the differences between the ω ln,HOMO and ω ln,LUMO values significantly increase with an increase in molecular size in B, N-substituted polyacene-series. Such different properties in the ω ln,HOMO and ω ln,LUMO values between polyacene-series and B, N-substituted polyacene-series may come from the electronegativity perturbation on polyaceneseries. The ω ln,HOMO values for polyacene-series are larger than those for B, Nsubstituted polyacene-series. This is because only the C–C stretching modes around 1500 cm–1 play an essential role in the electron–phonon interactions in polyacene-series, while the low frequency modes as well as the B–N stretching modes around 1500 cm–1 play an important role in the electron–phonon interactions in B, N-substituted polyacene-series. The results for the ω ln,HOMO values in B, N-substituted polyacene-series are not in agreement with a tendency in solids, as described above. That is, the electronic structures rather than the molecular weights are closely related to the frequencies of the vibrational modes which play an important role in the electron–phonon interactions in the monocations of B, N-substituted polyacene-series. The ω ln,HOMO value increases with an increase in molecular size from 1a to 2a, but the ω ln,HOMO value slightly decreases with an increase in molecular size from 2a to 6a. On the other hand, the ω ln,HOMO values for B, N-substituted polyacene-series increase with an increase in molecular size from 1bn to 3bn. But from analogy with the calculated results for polyacene-series, the ω ln,HOMO values may begin to decrease at the finite size of B, N-substituted polyacene-series, according to the general tendency in solids; light mass will lead to higher values of ω ln .


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C. Polycyanodienes The ω ln,HOMO values are estimated to be 1015, 1002, and 1009 cm–1 in 2cn, 3cn, and 4cn, respectively. Those are estimated to be 1521, 1501, and 1450 cm–1 in 2a, 3a, and 4a, respectively. Therefore, the ω ln,HOMO values do not significantly change with an increase in molecular size in polycyanodienes. Furthermore, the ω ln,HOMO values for polycyanodienes are smaller than those for polyacenes. The ω ln,LUMO values are estimated to be 1179, 1381, 1242, and 1150 cm–1 for 1cn, 2cn, 3cn, and 4cn, respectively, and those are estimated to be 1390, 1212, 1023, and 926 cm–1 for 1a, 2a, 3a, and 4a, respectively. Therefore, apart from 1cn, the ω ln,LUMO values for polyacenes and polycyanodienes decrease with an increase in molecular weights. This is in qualitative agreement with a tendency; light mass will lead to higher values of ω ln . But it should be noted that the ω ln,LUMO values for polycyanodienes with D2h geometry are larger than those for

polyacenes with D2h geometry. As described above, the LUMO of polyacenes is rather localized on carbon atoms located at the edge part of carbon framework in polyacenes, and thus the non-bonding characteristics are significant. Therefore, the orbital interactions between two neighboring carbon atoms are weak. On the other hand, due to electronegativity perturbation, the LUMO of polycyanodienes is delocalized, and the electron density on carbon atoms as well as on nitrogen atoms located at the edge part of CN framework is high, and thus the orbital interactions between two neighboring carbon and nitrogen atoms and between two neighboring carbon atoms in the LUMO are strong. This is the reason why the C– N and C–C stretching modes around 1500 cm–1 in the monoanions of polycyanodienes afford larger electron–phonon coupling constants than the C–C stretching modes around 1500 cm–1 in the monoanions of polyacenes, and the reason why the ω ln,LUMO values for polycyanodienes are larger than those for polyacenes. Therefore, the orbital patterns difference between the delocalized LUMO in polycyanodienes and the LUMO localized on carbon atoms located at the edge part of carbon framework in polyacenes is the main reason why the lLUMO and ω ln,LUMO for polycyanodienes are larger than those for polyacenes.

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D. Summary In this chapter, we investigated the logarithmically averaged phonon frequencies which measure the frequencies of the vibronic active modes playing an essential role in the electron–phonon interactions in polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes. The ω ln,HOMO and ω ln,LUMO values decrease with an increase in molecular size in polyacenes and polyfluoroacenes. This is in qualitative agreement with a tendency in conventional superconductors; light mass will lead to higher values of ω ln . The ω ln,HOMO values for polyfluoroacenes become smaller than those for polyacenes

by H–F substitutions. The ω ln,LUMO values for polyfluoroacenes decrease with an increase in molecular size less rapidly than those for polyacenes. The ω ln,LUMO values for 1fa, 2fa, and 3fa become smaller than those for 1a, 2a, and 3a, by H–F substitutions. However, considering the large Mw values difference between 1fa and 1a, 2a and 2fa, and 3a and 3fa, the ω ln,LUMO values difference between polyacenes and polyfluoroacenes is not large. Furthermore, the ω ln,LUMO values for 4fa and 5fa are larger than those for 4a and 5a even though the Mw values for 4fa and 5fa are larger than those for 4a and 5a, respectively. We can expect that in the hydrocarbon molecular systems, the ω ln values would basically decrease by substituting hydrogen atoms by heavier atoms. This can be understood from the fact that the frequencies of all vibronic active modes in polyacenes downshift by H–F substitution. However, considering that the ω ln value for the LUMO rather localized on carbon atoms in 4fa and 5fa becomes larger by H–F substitution, we can expect that the ω ln value for a molecular orbital localized on carbon atoms has a possibility to increase by substituting hydrogen atoms by heavier atoms if the phase patterns of the molecular orbital do not significantly change by such atomic substitution. Therefore, the detailed properties of the vibrational modes and the electronic structures as well as the molecular weights are closely related to the frequencies of the vibronic active modes playing an important role in the electron–phonon interactions in the monoanions of polyfluoroacenes. The ω ln,HOMO values are larger than the ω ln,LUMO values in polyfluoroacenes. The significant phase patterns difference between the HOMO and LUMO is the main reason why the frequencies of vibronic active modes playing an essential role in the electron–phonon interactions in the monocations are significantly different from those in the monoanions in 2fa, 3fa, 4fa, and 5fa. Therefore, the detailed


71

properties of the vibrational modes and the electronic states as well as the molecular weights are closely related to the frequencies of the vibronic active modes playing an important role in the electron–phonon interactions in charged polyfluoroacenes. The ω ln,HOMO and ω ln,LUMO values, increase and significantly decrease, respectively, with an increase in molecular size in B, N-substituted polyacenes. As in polyacenes, the ω ln,HOMO values are larger than the ω ln,LUMO values in large size of B, N-substituted polyacenes. As in 1a, the ω ln,HOMO value is slightly larger than the ω ln,LUMO value in 1bn. The differences between the ω ln,HOMO and ω ln,LUMO values become larger with an increase in molecular size in

B, N-substituted polyacenes, while those in polyacenes hardly change. Such different properties in the ω ln,HOMO and ω ln,LUMO values between polyacenes and B, N-substituted polyacenes may come from the electronegativity perturbation on polyacenes. The ω ln,HOMO values for polyacenes are larger than those for B, Nsubstituted polyacenes. The results for the ω ln,HOMO values in B, N-substituted polyacenes are not in agreement with a tendency in solids, as described above. That is, the electronic structures rather than the molecular weights are closely related to the frequencies of the vibrational modes playing an important role in the electron–phonon interactions in the monocations of B, N-substituted polyacenes. The ω ln,HOMO values do not significantly change with an increase in molecular size in polycyanodienes. Furthermore, the ω ln,HOMO values for polycyanodienes are smaller than those for polyacenes. Apart from 1cn, the ω ln,LUMO values for polyacenes and polycyanodienes decrease with an increase in molecular weights. The ω ln,LUMO values for D2h symmetric polycyanodienes are larger than those for

D2h symmetric polyacenes. The phase patterns difference between the delocalized LUMO in polycyanodienes and LUMO localized on carbon atoms located at the edge part of carbon framework in polyacenes is the main reason why the ω ln,LUMO values for polycyanodienes are larger than those for polyacenes.

Chapter VIII

CONCLUDING REMARKS In this book, we discussed the electron–phonon interactions in the charged molecular systems such as polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes. We estimated the electron–phonon coupling constants and the frequencies of the vibronic active modes playing an essential role in the electron–phonon interactions. These physical values are essential to discuss several physical phenomena such as intramolecular electrical conductivity, intermolecular charge transfer, attractive electron–electron interactions and Bose–Einstien condensation, and superconductivity, which will be discussed in detail in the next review article. Motivated by the possible inverse isotope effects in Pd-H, Pd-D, and Pd-T superconductivity, and organic superconductivity observed by Saito et al., we discussed how the H–F substitution are closely related to the essential characteristics of the electron–phonon interactions in these molecules by comparing the calculated results for charged polyacenes with those for charged polyfluoroacenes, since fluorine atoms are much heavier than D and T atoms, and the phase patterns of the frontier orbitals such as the HOMO and LUMO are not expected to be significantly changed. Furthermore, we discuss how CC–BN and CC–CN substitutions are closely related to the essential characteristics of the electron–phonon interactions in these molecules by comparing the calculated results for charged polyacenes with those for charged B, N-substituted polyacenes and polycyanodienes, respectively. These physical values are essential to discuss the several physical phenomena such as intramolecular electrical conductivity, intermolecular charge transfer, attractive electron–electron interactions and Bose–Einstien condensation, and superconductivity, which will be discussed in detail in the next review article.

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In this review article, we investigated the electron–phonon interactions in the monocations and monoanions of polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes. The C–C stretching modes around 1500 cm–1 strongly couple to the HOMO, and the lowest frequency modes and the C–C stretching modes around 1500 cm–1 strongly couple to the LUMO in polyacenes. The C–C stretching modes around 1500 cm–1 strongly couple to the HOMO and LUMO in polyfluoroacenes. The B–N stretching modes around 1500 cm–1 strongly couple to the HOMO and LUMO in B, N-substituted polyacenes. The C– C and C–N stretching modes around 1500 cm–1 strongly couple to the HOMO and LUMO in polycyanodienes. We estimated the total electron–phonon coupling constants in the monocations and monoanions of polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes. The lHOMO and lLUMO values decrease with an increase in molecular size in polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes. In general, we can expect that monocations and monoanions, in which number of carriers per atom is larger, affords larger lHOMO value. The lHOMO and lLUMO values for polyfluoroacenes are larger than those for polyacenes. The lHOMO values for B, N-substituted polyacenes are larger than those for polyacenes. The lLUMO values for B, N-substituted polyacenes are similar to those for polyacenes. The lLUMO values are larger than the lHOMO values in polyacenes, polyfluoroacenes, and B, N-substituted polyacenes. Therefore, electron doping rather than hole doping is more effective way to seek for large electron–phonon coupling constants in polyacenes, polyfluoroacenes, and B, Nsubstituted polyacenes. Both the lHOMO and lLUMO values for polycyanodienes are larger than those for polyacenes. Therefore, CH–CF, CC–BN, and CC–CN atomic substitutions are effective way to seek for large lHOMO and lLUMO values in polyacenes. The orbital patterns difference between the LUMO localized on carbon atoms located at the edge part of carbon framework in polyacenes and the delocalized LUMO in polycyanodienes due to electronegativity perturbation, is the main reason why the lLUMO values for polycyanodienes are much larger than those for polyacenes. Strong σ orbital interactions between two neighboring carbon atoms and two neighboring carbon and nitrogen atoms and the orbital interactions between two neighboring carbon and hydrogen atoms in the HOMO of polycyanodienes are the main reason why the lHOMO values for σ-conjugated polycyanodienes are much larger than those for π-conjugated polyacenes. The lHOMO values are larger than the lLUMO values in polycyanodienes. Strong σ

Concluding Remarks

75

orbital interactions between two neighboring carbon atoms and two neighboring carbon and nitrogen atoms and the orbital interactions between two neighboring carbon and hydrogen atoms in the HOMO and the weak π orbital interactions between two neighboring carbon atoms and two neighboring carbon and nitrogen atoms in the LUMO of polycyanodienes, are the main reason why the lHOMO values are larger than the lLUMO values in polycyanodienes. We also investigated the logarithmically averaged phonon frequencies which measure the frequencies of the vibronic active modes playing an essential role in the electron–phonon interactions in polyacenes, polyfluoroacenes, B, N-substituted polyacenes, and polycyanodienes. The ω ln,HOMO and ω ln,LUMO values decrease with an increase in molecular size in polyacenes and polyfluoroacenes. This is in qualitative agreement with a tendency in conventional superconductors; light mass will lead to higher values of ω ln . The ω ln,HOMO values for polyfluoroacenes become smaller than those for polyacenes by H–F substitutions. The ω ln,LUMO values for polyfluoroacenes decrease with an increase in molecular size less rapidly than those for polyacenes. The ω ln,LUMO values for 1fa, 2fa, and 3fa become smaller than those for 1a, 2a, and 3a, by H–F substitutions. However, considering the large Mw values difference between 1fa and 1a, 2a and 2fa, and 3a and 3fa, the ω ln,LUMO values difference between polyacenes and polyfluoroacenes is not large. Furthermore, the ω ln,LUMO values for 4fa and 5fa are larger than those for 4a and 5a even though the Mw values for 4fa and 5fa are larger than those for 4a and 5a, respectively. We can

expect that in the hydrocarbon molecular systems, the ω ln values would basically decrease by substituting hydrogen atoms by heavier atoms. This can be understood from the fact that the frequencies of all vibronic active modes in polyacenes downshift by H–F substitution. However, considering that the ω ln value for the LUMO rather localized on carbon atoms in 4fa and 5fa becomes larger by H–F substitution, we can expect that the ω ln value for a molecular orbital localized on carbon atoms has a possibility to increase by substituting hydrogen atoms by heavier atoms if the phase patterns of the molecular orbital do not significantly change by such atomic substitution. Therefore, the detailed properties of the vibrational modes and the electronic structures as well as the molecular weights are closely related to the frequencies of the vibronic active modes playing an important role in the electron–phonon interactions in the monoanions of polyfluoroacenes. The ω ln,HOMO values are larger than the ω ln,LUMO values in polyfluoroacenes. The significant phase patterns difference between the HOMO and LUMO is the main

76

Takashi Kato

reason why the frequencies of vibronic active modes playing an essential role in the electron–phonon interactions in the monocations are significantly different from those in the monoanions in 2fa, 3fa, 4fa, and 5fa. Therefore, the detailed properties of the vibrational modes and the electronic states as well as the molecular weights are closely related to the frequencies of the vibronic active modes playing an important role in the electron–phonon interactions in charged polyfluoroacenes. The ω ln,HOMO and ω ln,LUMO values, increase and significantly decrease, respectively, with an increase in molecular size in B, N-substituted polyacenes. As in polyacenes, the ω ln,HOMO values are larger than the ω ln,LUMO values in large size of B, Nsubstituted polyacenes. As in 1a, the ω ln,HOMO value is slightly larger than the ω ln,LUMO value in 1bn. The differences between the ω ln,HOMO and ω ln,LUMO values become larger with an increase in molecular size in B, N-substituted polyacenes, while those in polyacenes hardly change. Such different properties in the ω ln,HOMO and ω ln,LUMO values between polyacenes and B, N-substituted polyacenes may come from the electronegativity perturbation on polyacenes. The ω ln,HOMO values for polyacenes are larger than those for B, N-substituted polyacenes. The results for the ω ln,HOMO values in B, N-substituted polyacenes are not in agreement with a tendency in solids, as described above. That is, the electronic structures rather than the molecular weights are closely related to the frequencies of the vibrational modes playing an important role in the electron–phonon interactions in the monocations of B, N-substituted polyacenes. The ω ln,HOMO values do not significantly change with an increase in molecular size in polycyanodienes. Furthermore, the ω ln,HOMO values for polycyanodienes are smaller than those for polyacenes. Apart from 1cn, the ω ln,LUMO values for polyacenes and polycyanodienes decrease with an increase in molecular weights. The ω ln,LUMO values for D2h symmetric polycyanodienes are larger than those for D2h symmetric polyacenes. The phase patterns difference between the delocalized LUMO in polycyanodienes and LUMO localized on carbon atoms located at the edge part of carbon framework in polyacenes is the main reason why the ω ln,LUMO values for polycyanodienes are larger than those for polyacenes. In summary, CH–CF, CC–BN, and CC–CN atomic substitutions are effective way to seek for larger lHOMO values, and CH–CF and CC–CN atomic substitutions are effective way to seek for larger lLUMO values in polyacenes.

ACKNOWLEDGMENT This study was performed under the Project of Academic Frontier Center at Nagasaki Institute of Applied Science. This work is partly supported by a Grantin-Aid for Scientific Research from the Japan Society for the Promotion of Science (JSPS-16560618, JSPS-17350094).

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INDEX A amplitude, 18, 28, 29 atomic orbitals, 21, 23, 26, 38 atoms, viii, 4, 21, 23, 26, 28, 31, 33, 34, 35, 36, 37, 38, 39, 42, 43, 44, 45, 46, 50, 52, 53, 56, 57, 58, 59, 60, 66, 69, 70, 73, 74, 75

B BCS theory, 2 bending, 27, 31, 39 benzene, 18, 19, 25 bonding, 21, 28, 31, 32, 34, 35, 37, 38, 39, 42, 43, 44, 45, 56, 59, 69 bonds, 16, 26, 39

compensation, 37, 38 condensation, 4, 73 conductivity, 4, 73 consensus, 1 control, 1 couples, 28, 31, 33, 34, 35, 36, 37, 38, 40, 42, 43, 45, 46, 52 coupling, vii, 1, 2, 4, 5, 6, 7, 8, 9, 10, 11, 12, 15, 16, 17, 18, 19, 27, 28, 29, 30, 31, 32, 33, 34, 36, 37, 39, 40, 41, 42, 43, 44, 46, 49, 50, 51, 53, 55, 57, 58, 60, 69, 73, 74 coupling constants, vii, 2, 4, 6, 7, 9, 10, 11, 12, 15, 16, 27, 29, 30, 31, 32, 33, 34, 37, 39, 40, 41, 42, 43, 44, 46, 49, 50, 51, 53, 55, 57, 58, 60, 69, 73, 74 crystals, 1, 2, 15

D C carbon, viii, 21, 23, 25, 26, 28, 31, 32, 34, 35, 36, 37, 38, 43, 44, 45, 47, 50, 52, 53, 56, 57, 58, 59, 60, 66, 69, 70, 74, 75 carbon atoms, viii, 21, 23, 28, 31, 32, 34, 35, 36, 37, 38, 45, 50, 52, 53, 56, 57, 59, 60, 66, 69, 70, 74, 75 carbon nanotubes, 25 cation, 23 cell, 17 C-N, 25

deformation, 1 degenerate, 1, 7, 9, 10, 18, 25 density, 16, 21, 23, 26, 38, 40, 50, 53, 56, 57, 59, 60, 66, 69 derivatives, 7, 27 DFT, 21, 27 diamonds, 51, 64 distortions, 57 doping, 60, 74

Index

86

E electrical conductivity, 1, 4, 73 electron density, 23, 38, 56, 59 electronic structure, viii, 52, 66, 67, 68, 70, 75 electronic systems, 1 electron–phonon interactions, vii, 1, 2, 4, 37, 38, 42, 50, 60, 67, 68, 70, 73, 75 electrons, 1, 5 energy, 5, 6, 8, 9, 10, 12, 19, 21, 23, 25, 26, 27, 28, 31, 33, 34, 35, 37, 38, 40, 42, 43, 45, 56, 57 equilibrium, 7, 16, 17, 19, 27 exciton, 1 expectations, 2 expression, 2, 16 extrapolation, 53

F Fermi level, 1, 16, 17 fluorine, 4, 23, 31, 32, 34, 35, 36, 37, 38, 52, 66, 73 fluorine atoms, 4, 23, 31, 32, 34, 35, 36, 37, 38, 52, 66, 73 France, 79

H Hamiltonian, 5 hybrid, 21, 27 hydrides, 2 hydrocarbons, 21 hydrogen, viii, 1, 2, 26, 36, 40, 43, 44, 52, 57, 58, 61, 66, 70, 74, 75 hydrogen atoms, viii, 26, 36, 40, 43, 44, 52, 57, 58, 61, 66, 70, 74, 75 hypothesis, 2

I instability, 1 interaction, 1, 8, 21, 42

interactions, vii, 1, 2, 4, 5, 10, 15, 16, 21, 26, 28, 31, 32, 34, 35, 37, 38, 39, 42, 43, 44, 45, 46, 47, 50, 53, 56, 57, 58, 59, 60, 63, 66, 67, 68, 69, 70, 73, 74, 75 ionization, 2 isotope, 1, 2, 4, 73

J Japan, 77

M mass, 31, 35, 36, 40, 46, 65, 68, 69, 70, 75 matrix, 5, 7, 8, 10, 12, 16, 17, 18, 19 mode, 1, 7, 8, 9, 10, 11, 12, 15, 16, 17, 18, 19, 27, 28, 31, 32, 34, 35, 36, 37, 38, 39, 40, 41, 43, 44, 45, 46, 50, 54, 65 molecular structure, 1 molecular weight, viii, 63, 64, 66, 67, 68, 69, 70, 75 molecules, vii, 1, 4, 16, 17, 21, 23, 73

N naphthalene, 2, 25 neglect, 17 New York, iv nitrogen, 25, 26, 45, 47, 57, 58, 59, 61, 69, 74 nitrogen compounds, 25 nuclei, 5

P pairing, 15 palladium, 2 phonons, 1 photoelectron spectroscopy, 2 physical properties, 23 physics, 1 polarizability, 23 polyacenes, vii, 2, 4, 5, 6, 7, 11, 12, 13, 16, 17, 20, 21, 22, 23, 24, 25, 26, 27, 29, 30,

Index 36, 37, 40, 41, 42, 47, 49, 50, 51, 52, 54, 55, 56, 57, 58, 59, 60, 63, 64, 65, 66, 69, 70, 73, 74, 75, 76 polycyanodienes, vii, 4, 5, 6, 7, 13, 16, 17, 20, 22, 24, 26, 44, 46, 47, 49, 51, 57, 58, 59, 60, 63, 64, 69, 70, 73, 74, 75 prediction, 1 pressure, 2 program, 21 pyrolysis, 25

R range, 27 resolution, 2

superconductor, 1 symmetry, 7, 11, 23, 25, 26 synthesis, 1 systems, vii, 1, 2, 4, 15, 23, 66, 70, 73, 75

T theory, 1, 2, 16, 21, 26, 31 thermolysis, 25 time, 23 total energy, 7 transformations, 19 transition, 1, 2 transition temperature, 1, 2 transport, 2

S scattering, 15 series, 39, 42, 43, 53, 55, 56, 58, 59, 67, 68 shape, 23 sign, 23 spectroscopy, 1 spin, 16, 18 stabilization, 36, 38 stretching, vii, 27, 28, 31, 34, 35, 36, 37, 39, 40, 41, 42, 43, 44, 46, 47, 50, 52, 53, 54, 55, 57, 60, 65, 66, 67, 68, 69, 74 substitution, viii, 2, 4, 23, 25, 37, 52, 65, 66, 70, 73, 75 superconductivity, 1, 2, 4, 15, 73

87

V values, vii, 4, 15, 49, 50, 51, 52, 53, 55, 56, 57, 58, 59, 60, 63, 64, 65, 66, 67, 68, 69, 70, 73, 74, 75, 76 variation, 21, 23, 26 vibration, 8, 11

W wave number, 27 wave vector, 16, 17 workers, 25

Electron-Phonon Interactions in Novel Nanoelectronics

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